Every machine in every lab falls into one of three categories. The category tells you who has to be standing there before you switch it on.
Three categories, one question
Three categories, one question
Every piece of equipment in the lab is Category 1, 2 or 3. The
category answers one question: who has to be present before you switch it on?
Permission from an instructor is required in every case. What changes between categories is
when that permission can be given, and who has to be in the room while the machine is running.
Category 1
Permission may be given in advance. Work alone once you have it.
Category 2
Permission at the time of use. A peer must be present throughout.
Category 3
Permission at the time of use. A peer and an instructor must be present throughout.
Power down safely — turn off and disconnect the equipment from its power source.
Report issues immediately — notify the instructor of any broken or malfunctioning equipment.
Return and organize — put all equipment and tools back in their designated locations.
Restore to shutdown state — return the equipment to its original, safe configuration.
Clean thoroughly — remove all dust, chips, liquids and debris from the equipment and the work area.
The habit behind the last two is 5S — the same discipline,
named and made routine.
Safety/Universal Rules
Personal Protective Equipment
What you wear, and when. Eye protection is mandatory in the lab spaces at all times; the rest depends on the task.
Personal Protective Equipment
Personal Protective Equipment
Five topics. One of them — eye protection — applies the moment you walk
in. The rest are set by what you are doing.
Eyes
Always, in the lab spaces. No exceptions.
Hearing
Prolonged exposure to loud equipment.
Feet
Closed-toe shoes, always.
Respiratory
Any grinding or sanding; hazardous dust or fumes.
Clothing & hair
Always, near anything that rotates.
Eye protection; Watch out
Eye protection
Safety glasses are MANDATORY in the lab spaces at all times.
If you wear prescription glasses
Side shields that attach to your existing frames.
Oversized safety glasses that fit over corrective glasses.
Prescription safety glasses are also acceptable.
Lens requirements
Safety glasses must be clear or yellow tinted only.
Dark or shaded safety glasses are not acceptable for indoor lab use.
Must meet ANSI Z87.1 safety standards.
Hearing protection; Watch out
Hearing protection
Industry standard: shop tools nearly always require hearing protection in
professional settings. In a teaching lab the exposure is typically shorter than in production
work, but the protection still matters.
When to use it
Required for prolonged exposure to loud equipment — grinders, sanders, planers and similar.
The rule of thumb: if you have to raise your voice to be heard by someone at arm’s
length, it is loud enough to need protection. You do not need a meter, and most shop
tools fail this test the moment they start.
The numbers behind it
OSHA measures noise as an average across the working day, in A-weighted decibels
(dBA). Two figures matter:
85 dBA
The action level, averaged over 8 hours — the point at which a workplace must run a hearing conservation programme.
90 dBA
The permissible exposure limit, averaged over 8 hours.
Above 90 dBA the allowed time drops fast — every extra 5 dBA halves it:
90 dBA
8 hours
95 dBA
4 hours
100 dBA
2 hours
105 dBA
1 hour
110 dBA
30 minutes
115 dBA
15 minutes or less
Impact noise should not exceed 140 dB peak — a single hammer blow or
nail gun can reach it, and that damage is immediate rather than cumulative.
These are OSHA workplace limits (29 CFR 1910.95). NIOSH recommends a stricter
85 dBA limit that halves the allowed time every 3 dBA rather than every 5. Hearing loss
from noise does not come back, so treat these as ceilings, not targets.
Two types available
Earplugs
Small foam plugs inserted into the ear canal. Disposable or reusable. Available on request from the instructor.
Ear muffs
Over-ear cups covering the whole ear. Reusable and adjustable. Often preferred for intermittent use.
Both types significantly reduce harmful noise levels.
Foot protection
Foot protection
Minimum requirement: closed-toe shoes are MANDATORY — no sandals, no flip-flops, no open-toe footwear.
Recommended upgrades
Slip-resistant soles, for traction on surfaces that may be slippery.
Puncture-resistant soles, against sharp metal debris.
Steel-toe or composite-toe protection — recommended, not required.
Avoid
Canvas shoes or thin-soled footwear.
High heels or unstable footwear.
Anything that does not fully enclose your feet.
You will be standing for most of the lab period — choose something
supportive and comfortable.
Respiratory protection; Stop
Respiratory protection
MANDATORY when using any grinder or sander, and when working with materials
that produce hazardous dust.
Grinding galvanized material is PROHIBITED. Zinc fumes from galvanized steel
are toxic when heated.
Health hazards
Metal dust and particles cause respiratory irritation and long-term lung damage.
Wood dust can cause allergic reactions.
Dust and fumes are not the same problem, and they do not take the
same protection. The next section is the one that decides which you need.
Respiratory protection — what to wear; Stop; Watch out
Respiratory protection — what to wear
A dust mask does nothing against fumes or vapours. An N95 is a
particle filter. It does not stop gases, welding or brazing fume, solvent vapour, or
anything else you can smell. Wearing one while you can smell the air is not protection.
For dust — grinding, sanding, sawing
N95 mask
Filters 95% of airborne particles. The minimum for dusty work.
Half- or full-face respirator
Fitted with a particulate filter, for heavy or extended dust.
For fumes and vapours
You need an approved respirator with the right chemical cartridge, not a
dust mask. Ask the instructor which cartridge before you start.
A respirator only works if it seals. A loose mask, or a beard along the
seal, defeats it.
If there is no correct cartridge available, the job does not happen until
there is.
If you can smell fumes or taste particles, your protection is inadequate.
Stop work immediately and upgrade it — or stop the job.
Loose clothing and accessories catch in rotating machinery. That is how this
causes serious injury or death — it is not a dress code.
Prohibited
Loose-fitting clothing, or garments with dangling features — drawstrings, ties and similar.
Long sleeves, hoodies or jackets near rotating equipment.
ALL jewelry, except silicone wedding rings.
Neckties, scarves and lanyards.
Hair, and what to wear instead
Hair, and what to wear instead
Hair
Long hair must be secured back and kept away from equipment.
Use hair ties, clips or caps to prevent entanglement.
Recommended
Cotton or fire-retardant materials — preferred, not required.
Close-fitting, short-sleeved shirts.
Pants without excessive loose material.
Safety/Universal Rules
Lifting and Carrying
Team lifting above 40 lbs, and the technique that keeps you in control of the load. What usually defeats a lift is the size of the thing, not its weight.
Lifting Rules; Watch out
Lifting Rules
Get a second person for anything over 40 lbs. A gym weight plate is
45 lbs and nobody lifts one in pairs. Size — not weight — is what makes shop
materials hard to carry.
Forty pounds of aluminum bar is about four inches square and two feet long: you can hold it
against your chest, see over it, and set it down where you meant to. A twenty-foot piece of tube
can weigh less than that and still put half its length out in front of you, and a sheet of
plywood fills your arms and hides the floor you are walking on. Same weight, different job.
OSHA sets no weight limit — no standard says how much a person may
lift, only that a workplace be kept free of recognized hazards. The number everyone borrows
comes from NIOSH, the federal institute that researches workplace injury:
51 lbs with two hands under ideal conditions, cut for every way a real
lift is worse. Hold that same load at arm's length instead of against you and it rates about
20 lbs. Turning a quarter circle as you lift takes off another 30%, and
nothing good to grab takes off 10% more. A load much wider than your body is outside what the equation covers
at all — used there, it underestimates the hazard.
Team lifting is required for
Anything over 40 lbs.
Items lighter than 40 lbs but awkward in shape, size or balance.
Any object that feels unstable or is difficult to grip.
The 40 lb line is as much about dropping it as about your back.
A load you cannot fully control is a hazard to your feet, the floor, the workpiece and anyone
walking past — well before it is a hazard to your spine.
If you cannot hold it against your body and keep your back straight, it is too heavy
for you to lift alone — whatever the number says. Weight still wins in the end;
that point just sits somewhere different for every person and every shape.
Proper lifting technique; Checklist
Proper lifting technique
Plan the lift — clear your path and know where you are going.
Get close to the object before lifting.
Squat down using your leg muscles; keep your back straight.
Grip firmly with both hands; avoid awkward hand positions.
Lift smoothly using your legs, not your back.
Keep the load close to your body throughout the lift.
Setting it down
Use the same technique in reverse — squat down, do not bend over.
Place objects gently. Do not drop them.
Safety/Universal Rules
Electrical Safety
Why 50 V is a workplace control threshold, why 5 V can still burn you, the inspection required before every use, cords on the floor, and what to do when someone is shocked.
Electrical Sources
Electrical Sources
What hurts you at 5 V is not what hurts you at 240 V; one is a burn hazard
while the other is a shock hazard.
5 V / 12 V
The power supply on the bench, batteries, and the battery
pack out of a cordless drill. Lower shock risk, not a magic cutoff. Not below the
burn threshold.
120 V
Wall outlets. Dangerous — can cause serious injury or
death.
240 V / 480 V
Industrial equipment. Extremely dangerous — often
fatal.
Voltage tells you whether a circuit can push current through you. It does
not tell you what that circuit can do to a ring, a dropped tool or a shorted cell.
Those are two different hazards with two different thresholds. The next two sections are
about how each hazard changes.
Electrical — Shock Hazard; Stop
Electrical — Shock Hazard
There is no magic voltage at which shock suddenly becomes possible. A shock can be
painful without being life-threatening, and its severity depends on current, path, duration, and
your body’s resistance. Higher voltage can drive more current through the body, so the risk of
serious injury rises with it. In U.S. workplace rules, 50 volts is a common
control threshold: at or above it, live parts must be guarded and work near exposed live parts
requires specific controls.
OSHA requires live parts to be de-energized before you work on or near them — and then
says that “live parts that operate at less than 50 volts to ground need not be
deenergized if there will be no increased exposure to electrical burns or to explosion due to
electric arcs” (29 CFR 1910.333(a)(1)). Read that second
half again; the rest of this page hangs on it.
At or above the line, live parts must be guarded against accidental contact.
The rule is written for “electric equipment operating at 50 volts or more”
(29 CFR 1910.303(g)(2)(i)).
That number applies to DC as well as AC. The standard does not distinguish
between them, and OSHA has stated it “considers all voltages of 50 volts or above to be
hazardous” (interpretation letter, 4 September 2015).
NFPA 70E draws the same line. Below 50 V you may work live only where the
capacity of the source and any overcurrent protection have been considered and found
not to add burn or arc exposure (2024 edition, 110.2(B) Exception No. 5).
Supporting detail: Addendum 1 — “It’s not the voltage that gets you, it’s the current”.
Supporting detail: Addendum 2 — The international standards are not one number.
In this lab, use 50 V — AC or DC. It is the number OSHA enforces,
it is the most conservative of the figures above, and it assumes nothing about your skin being
dry or your hands being clean. If a circuit is at or above 50 V, it is not something you
work on live.
Electrical — Burn Hazard; Stop
Electrical — Burn Hazard
Below 50 V, the primary concern often shifts from shock to
short-circuit current. This is the half of the page people get wrong, because the
voltage people assume is harmless is the one nobody is careful with.
Look at what the exemption above is actually conditioned on. Not shock — burns
and arcs. NFPA 70E names the same condition as the capacity of the source.
Both standards are telling you that once you are under that workplace control threshold, the
question changes from how many volts to how many amps can this thing deliver into
a dead short.
Where the current comes from
A bench supply set to 5 V will deliver its full rated current into a
short without complaint. That is what the current limit is for — and if you have wound the
limit up to get a motor turning, you have wound the protection off.
A lithium cell or pack has almost no internal resistance. Shorted, a single
cell can dump tens of amps within milliseconds. A pack does considerably worse.
A lead-acid battery is rated in hundreds of cold-cranking amps — and
that is a 30-second load test, not a ceiling. A dead short pulls far more.
None of these can push meaningful current through your body at 12 V. All of them can push
hundreds of amps through a piece of metal — and metal carrying current it was never sized
for gets hot, fast.
Metal jewelry is the classic way this happens
ALL jewelry is already PROHIBITED here — see
clothing and jewelry. That rule was written for rotating machinery. It earns its keep a
second time on the bench, and OSHA writes it a second time for exactly this reason: conductive
jewelry “may not be worn if they might contact exposed energized parts”
(29 CFR 1910.333(c)(8)) — a rule that states no voltage
floor. The same sentence gives the way out: such articles may be worn if they are
“rendered nonconductive by covering, wrapping, or other insulating means.”
A ring or a metal watch band bridging a low-voltage source is a near-zero-resistance path
across something that can supply hundreds of amps. The ring becomes the heating element. This is
documented injury, not a story: a mechanic’s gold ring touched the positive terminal of a
12 V car battery while the wrench in his hand bridged the ring and the
negative terminal, and the result was a deep circumferential burn around the base of the finger
that needed a skin graft. A review of nine ring burns at one burn center found the same pattern:
the small size of the burn hides how bad it is, because a burn that wraps a
finger is far more likely to need grafting and to leave lasting loss of function than a burn of
the same area anywhere else.
You can drop a wrench. You cannot drop a ring.
The silicone wedding ring that the PPE rule allows is also the right answer
electrically: silicone does not conduct, so it cannot become the short.
A shorted lithium cell does not just get warm
An external short is one of the recognized triggers for thermal runaway
— the cell generates heat faster than it can shed it, and the outcome is
“extremely high temperatures, violent cell venting, smoke and fire” (UL Research
Institutes). Once it has started, disconnecting it does not stop it. The cell is
now its own energy source.
NEVER leave loose cells or packs where metal can bridge the terminals
— a drawer with tools in it, a pocket with keys in it, a bin with offcuts in it. Federal
transport rules require lithium cells and batteries to be packed so their terminals cannot short
(49 CFR 173.185). The reason that rule exists is the reason to do the same
thing on your own bench.
A cell that has been shorted, dropped, crushed, punctured or has swollen is out of
service. Tell the instructor. Do not put it back on charge to find out. See
Fire Safety.
The sentence to take away: low voltage does not mean low energy.
Voltage helps determine whether a circuit can shock you. Current decides whether it can burn
you — and current is set by what the source can deliver and what is in the path,
not by the number printed on the front of the supply.
Electrical Conductors; Stop; Watch out; Checklist
Electrical Conductors
Inspect every cord, every time, before it goes into the receptacle.
Never run your hand along a cord while it is plugged in; that is a dangerous way to find fraying.
It takes about five seconds, and it is the one check that catches most of this page before it
happens rather than after.
With the cord unplugged, run it through your hand end to end. Look for frayed,
cracked, cut or exposed insulation, and for flat spots where something has been driven
over it.
Check the plug: blades all present, straight, tight in the body, not
discolored or pitted. Check the ground pin is still there — a missing
ground pin means the cord is out of service, not that you have found a workaround.
Check where the cord enters the plug and enters the tool. That is where
flexing breaks conductors, and it is where the damage hides.
Inspect extension cords for cuts, crushing and wear, and check the receptacle end for
scorching or melted plastic.
Damage like this means the cord is finished, not that it needs watching.
If you find damage, stop, unplug it, and notify the instructor. Not
“just for this one cut”. Tag it or hand it over, so the next person does not find it
the hard way.
Tape is not a repair. OSHA allows electrical tape over superficial scuffs in
the outer jacket, and has stated just as plainly that “tape repairs of the jacket may not
be used to bring a worn or frayed flexible cord into compliance” (interpretation letter,
16 December 1998). If conductors or their insulation are showing, the cord is done.
Connections and plugs
Always disconnect power before performing any maintenance or adjustment.
NEVER yank or pull a cord — grasp the plug, not the cord. Pulling by
the cord wrecks the strain relief where you cannot see it, and it is how a plug ends up
half out of the receptacle with the blades exposed.
Push a plug fully home, and look at it. A plug that will not seat is a
fault to report, not a fit problem to force.
Keep electrical connections away from water and wet surfaces. Wet skin has on the order of
1,000 ohms of resistance where dry skin has 100,000 ohms or
more, so water moves you roughly a hundredfold closer to the current every rule on this
page is trying to keep out of you.
Be aware of overhead wiring when you are handling long stock, moving a
ladder or lifting.
A partly unplugged appliance is a short waiting for something to land on it
The hazard is the gap, and it is there before anything lands in it.
Exposed blades sit at full line voltage with nothing between them but air. Anything
conductive that falls across them completes the circuit straight across the supply — and
in a shop, the thing that falls is a metal chip. What follows is not a shock.
It is a dead short: a bang, a hard flash, and enough heat at the contact point to weld and
pit the blades. It will very likely trip the breaker and it can wreck the outlet or whatever
is plugged into it. The breaker protects the wiring, not your face, and it does not act until
after the flash.
Plugs are all the way in or all the way out. Nothing in between, and nothing
left in between.
Chips travel further than you expect and they conduct — see
Metal Chips and Swarf. That is the direct line between the housekeeping rules and this one.
Cords on the floor — the one most likely to get you; Stop; Checklist
Cords on the floor — the one most likely to get you
Nothing else on this page is as likely to actually injure someone as a cord
lying across a walkway. It is not a shock hazard at all. It is a trip hazard
— and a trip in a shop is not a trip onto carpet. You land on concrete, or into a machine, or on something sharp.
The regulation treats this as a floor problem rather than an electrical one:
“walking-working surfaces are maintained free of hazards such as sharp or protruding
objects, loose boards, corrosion, leaks, spills, snow, and ice”
(29 CFR 1910.22(a)(3)), and passageways and work areas are kept “in a
clean, orderly, and sanitary condition” (29 CFR 1910.22(a)(1)). A cord
across an aisle is an obstruction in an aisle.
A trip in a shop is not a trip onto carpet. You land where the machines are.The correct route is longer and costs nothing. That is the whole argument.
What to do, in order of preference
Do not cross the walkway. Move the work to the outlet, or use a different
outlet. This is almost always available, and it is almost never the first thing anyone tries.
Route along the wall or the bench line rather than across open floor. Take
the long way around the edge of the room.
Go overhead where a drop or a reel is provided. That is what they are
for.
If it genuinely must cross, cover or anchor it. OSHA’s own guidance is
to “ensure that temporary electrical cords that cross aisles are taped or anchored to the
floor”. A cord ramp or cord cover does the same job better and protects the cord as well
as the person.
Use the shortest cord that reaches. Slack on the floor is the hazard, and a
coiled surplus in a walkway is the same hazard in a tighter package.
Unplug it and put it away when you are done, in the same movement as
shutting the tool down. The cord left out after the job is finished is the one nobody is
expecting.
PROHIBITED — running a flexible cord through a doorway, a window, or a hole in
a wall, ceiling or floor, and attaching it to building surfaces. Those are named
prohibitions in the electrical standard (29 CFR 1910.305(g)(1)(iv)),
along with using flexible cord as a substitute for the fixed wiring of a building. Flexible cord
is temporary by definition. A cord treated as permanent gets pinched, crushed and forgotten.
NEVER walk past a cord lying across a walkway and leave it because it is not
yours. If you can see it, you can move it or say something. The person who trips over it will
not have seen it.
Read from the cord’s side, the rule is the same: portable equipment must be
handled so it is not damaged, and every cord set must be inspected before use on any shift for
cuts, crushing and a pinched jacket (29 CFR 1910.334(a)). A cord that gets
walked on is a cord that fails the inspection above. This section and that one are the same
problem twice.
Keeping walkways clear is the Set in Order and Shine part of
5S. The safety case and the lean case are the same case.
If someone is shocked; Stop; Watch out
If someone is shocked
Do NOT touch them directly. If current is still flowing they are part of the
circuit, and grabbing them puts you in it as well.
Kill the power first — the machine switch, the disconnect, the
breaker, or pull the plug.
If you cannot kill it, use a dry, non-conductive object to separate them
from the source, and stand on something dry while you do it.
A small mark is not evidence of a small injury. Electrical and electrothermal
burns run deep with very little to see on the surface, and a burn that wraps a finger can cost
the use of it. Any shock, and any electrical burn, gets reported and gets looked at
— however fine the person says they are.
Safety/Universal Rules
Chemicals and Safety Data Sheets
Every chemical and liquid in the shop has a Safety Data Sheet. Read it before you use the material, not after.
What is a Safety Data Sheet (SDS)?
What is a Safety Data Sheet (SDS)?
A Safety Data Sheet is the manufacturer's written answer to
what their product can do to you, what to wear, and what to do when it goes wrong.
There are sixteen sections, always in the same order. You do not need to read a SDS front to
back but you should read the following three sections before you use a product.
Section 2
Hazard(s) identification. What the chemical can do
to you, in the manufacturer's own words — a signal word, the hazard statements, the
red-bordered pictograms.
Section 4
First-aid measures. On skin, in eyes, breathed in,
swallowed.
Section 8
Exposure controls / personal protection. Gloves,
eye protection, ventilation — the PPE answer for that specific chemical, rather
than the general one.
None of this is a local rule. OSHA requires a sheet for every hazardous chemical, and requires
the sixteen sections and the order they come in — 29 CFR 1910.1200(g).
Supporting detail: Addendum 3 — All sixteen sections, and the four OSHA does not enforce.
Supporting detail: Addendum 4 — Signal words, pictograms and H-numbers — how Section 2 is written.
Where is SDS binder located?
Where is SDS binder located?
All Safety Data Sheets are organized in a designated binder for easy reference.
Review before use — check the sheet for any unfamiliar chemical or liquid.
Ask the instructor if you cannot locate the sheet for a material.
The binder is one way of satisfying the rule underneath it.
1910.1200(g)(8) requires an employer to keep the sheets "readily accessible
during each work shift to employees when they are in their work area(s)", and allows
electronic copies in place of paper "as long as no barriers to immediate employee access in
each workplace are created by such options." Binder or screen, the test is the same: the
sheet is something you can reach now, not something you have to go and ask for.
Your responsibility: know the hazards of any chemical you are using, and
follow the proper handling procedures.
Supporting detail: Addendum 5 — Telling a current sheet from an old one.
Material Storage and incompatible materials
Material Storage and incompatible materials
Flammable liquids must be stored in an approved flammables cabinet when not in use.
NEVER store incompatible chemicals together.
All containers must be properly labeled.
“Incompatible” is not a judgement call, and answering it needs no
chemistry. It is written on the sheet, by name, in two places:
Section 10
Stability and reactivity. One of its required
entries is "incompatible materials" — what this chemical must not contact.
Beside it sit "conditions to avoid" and "hazardous decomposition products",
which is what the two of them would make.
Section 7
Handling and storage. Required to give
"conditions for safe storage, including any incompatibilities" — the same
question answered for the shelf rather than for the reaction.
So the test before two things share a cabinet: open both sheets and read Section 10 on
each. The entry may name a specific substance or a whole class of them — oxidizers,
strong acids. If either sheet names the other material, they do not go together. Read both,
because the pair may only be called out on one of them.
Supporting detail: Addendum 6 — What makes a flammables cabinet “approved”, and how to spot one.
Safety/Universal Rules
Machine Hazards and Housekeeping
The two ways a machine injures you - it catches hold and pulls you in, or it closes on you - plus the environment around it and the habits that keep both off you.
Rotating machinery; Stop; Watch out
Rotating machinery
Rotating machinery injures you by catching hold of something and pulling
it in. It does not have to catch your hand. It catches a sleeve, a glove, a lanyard or a
strand of hair, and your hand goes wherever that goes.
Gears, pulleys and belts, chains and sprockets are extremely dangerous.
Where a rotating part meets another surface there is a wedge that closes to nothing — an
in-running nip point, the place the machine feeds things into itself. It is
where the belt runs onto the pulley, where the chain runs onto the sprocket, where the gear
teeth mesh.
The contact and the injury happen in different places. You touch the belt out
in the open, where it looks like a moving strap; the belt carries you to the pulley, where there
is no gap at all. That distance is why staying clear of the nip point is not enough on its own
— anything the machine can grip is a handle it uses to bring you there.
Gloves. Gloves or rags are for handling sharp objects such as cutters, and
only once the machine is shut down. NEVER wear gloves at a running
machine — a glove catches where bare skin would pull free, and takes your hand
with it. See chips and gloves.
It does not take teeth, and it does not take speed. A plain smooth shaft turning
slowly will still wind hair or cloth onto itself, and once it has a turn or two it does not let
go.
Contact happens where the belt is open. The injury happens where it closes.
Supporting detail: Addendum 7 — The word for this, and where it comes from.
The rotating parts that have no cover
Belts, gears and chains belong behind covers. The working end of a machine does
not. The spindle — the driven shaft the motor turns — the
chuck that grips the tool or the work, and the stock (the raw
material) held in it all turn out in the open. Nothing is between you and them, because you have to
reach them to do the job.
So everything above about what gets caught applies here with nothing in the way — and it
applies to every machine that turns, not only the loud ones. A drill press is
quiet, it is slow, and it looks like the harmless one. It is still an open chuck spinning, and it
will wind hair, a sleeve or a glove onto itself like anything else. Slow is how long it
takes, not whether it happens.
The sleeve tore before the arm did. That is the shirt’s doing, not the machine’s.
The lathe is where this goes furthest, and the reason is what a lathe is. Most
machines hold the work still and move a cutter across it; a lathe does the opposite and
turns the work. What is spinning in the open is then not a bit the width of a
pencil — it is the whole part, as long and as heavy as that part happens to be. That is why
the fatality reports for lathes describe something other than a hand injury: a person wound onto
their own workpiece.
Wound on, cloth is a rope. Each revolution takes up another turn, and bracing changes nothing.
The question, before anything is switched on: what is turning, and what of mine can
reach it? A sleeve, a glove, loose hair and a strip of abrasive cloth held against the
work have each pulled somebody into a machine. Every one of them is easier to deal with before
the spindle is turning than after.
None of this is a ranking. The mechanism is the same on every machine that turns,
and the one that can catch you is whichever one you are standing at.
Supporting detail: Addendum 8 — What the investigations actually describe.
Moving machinery and pinch points; Watch out
Moving machinery and pinch points
Moving machinery injures you without ever catching hold of you.
Two surfaces close on each other with you in between. Nothing pulls you anywhere — you run
out of room.
What makes a pinch point
A pinch point is a gap that is closing: two parts, at least one of them
moving, with space between them that is on its way to nothing. That is the whole of it, and it is
why pinch points are hard to spot. There are no teeth, no edge and often no noise. A wide gap and
a narrow gap look the same until the last inch, and the gap does not care what is in it.
Two kinds of movement, and both make one:
Back and forth, up and down
A press ram, a drill head coming down, a saw guide
being lowered, a clamp closing. You are caught between the part that moves and the part that
does not.
Straight along
A table, a carriage or a saddle travelling. It closes the gap
against whatever waits at the end of its travel — a stop, a column, the machine’s
own frame, or the hand resting there.
Where they hide
Between the work and whatever holds it. A vise jaw, a clamp, a fixture: the
hand steadying the workpiece is inside the gap that is closing on the workpiece.
At the end of a table’s travel. Wind it far enough and the space
between the table and the frame goes to zero, with whatever was resting there in between.
Under anything that comes down. A head, a ram, a guard, a guide.
On hinges. Covers, doors and lids close on their own frames — at the
free edge, where a hand is holding them, and again right at the hinge, where the gap closes over
almost no distance at all.
A pinch point needs no power, no speed and no noise. A vise turned by hand
multiplies what you put into the handle many times over, and it closes slowly and quietly enough
that nothing warns you. Switching a machine off removes the part that would have closed the gap
for you. It does not remove the gap.
The question to ask
Before moving anything — a handwheel, a lever, a clamp, a guard —
what closes, and what is in the way? Follow the moving part to the end of its
travel and find what it meets there. Then look at where your hands are, and where they will still
be once you are watching the cut instead of watching your hands.
A pinch point is a gap on its way to zero. It looks safe for most of the trip.
Supporting detail: Addendum 9 — Why belts and chains count as rotating, not pinching.
Guards stay on, and taking one off is not your call; Stop
Guards stay on, and taking one off is not your call
A guard is the thing standing between you and everything the two sections above
describe. It is not an accessory, and it is not in your way — it is doing the one job
nothing else on the machine does.
No one removes a guard in this lab. A machine that needs a guard off is the
instructor’s to deal with, out of class.
That is the whole rule, and it is deliberately not a judgement call. You do not have to decide
whether this particular setup is the exception, whether the cut is short enough, or whether you
will be careful. If the guard is in the way, the answer is to stop and say so — not to
work out whether you can manage without it.
It also means a machine you find with a guard already missing is not ready to use.
Say something. You have not done anything wrong by finding it that way, and the person who uses it
after you has no way of knowing.
Supporting detail: Addendum 10 — Why the rule has no exceptions in it.
Lockout/Tagout — before anyone works on a machine; Stop
Lockout/Tagout — before anyone works on a machine
Everything on a machine that turns or travels does so because something is
powering it. Lockout/Tagout is how that power is taken away and kept away while somebody
works on the machine.
NEVER work on equipment with rotating or moving parts without first
disconnecting power.
Lockout/Tagout procedures must be followed for maintenance.
The two words
Lockout
A lock on the device that isolates the energy — the disconnect,
the breaker, the valve — so it physically cannot be switched back on.
Tagout
A tag on that same device saying who put it there and why, so nobody
removes it wondering.
Off is not disconnected, and disconnected is not still
Off is not disconnected. A machine’s own on/off switch is a control.
Someone can press it back on, and either way the machine is still connected to its supply. The
disconnect is the thing that gets locked.
Disconnected is not still. A spindle coasts. A raised head or ram drops. A
spring, a charged capacitor or air still in a line will all move something after the power is
gone. Energy already inside the machine is part of what the procedure has to deal with.
Supporting detail: Addendum 11 — What the standard actually covers.
The environment around the machine
The environment around the machine
Slip hazards
Clean dust, metal chips, water and coolant off the floor immediately.
Lighting
Ensure lighting is adequate before operating any machine.
Walkways
Keep aisles and emergency exits unobstructed.
Operating habits
Operating habits
The chuck key never leaves your hand. It is not released until it is out of
the chuck. There is no moment where the key is in the chuck and not in your grip — not to
reach for something, not to answer someone, not for a second.
Stop machines completely before taking measurements or making adjustments.
Secure all workpieces before operation — use clamps, vises or fixtures.
Never leave tools on or near operating machinery.
Supporting detail: Addendum 12 — Why the chuck key rule is worded as a grip and not as a reminder.
When to fight a fire and when to leave, and how to use an extinguisher.
Decide before you reach for anything; Stop; Checklist
Decide before you reach for anything
An extinguisher is for a small fire you caught early.
Fight it only if all four are true
The fire is small and contained — a bin, a rag, a puddle. Not spreading.
You know what is burning, and you have the right extinguisher for it.
You have a clear exit behind you and the fire is not between you and it.
Someone else has already raised the alarm.
Otherwise: get out. Pull the alarm, leave, call 911 from
outside, and tell the instructor and the fire crew what was burning.
If you try and it does not go out in the first few seconds, stop and leave.
A hand extinguisher lasts roughly 10–20 seconds. That is your whole attempt.
Using an extinguisher — PASS
Using an extinguisher — PASS
Remember the acronym: P–A–S–S.
When it looks out, back away watching the fire, exit behind
you. Do not assume it is over — a knocked-down fire can reignite.
Fire classes, and what puts them out
Fire classes, and what puts them out
Fires are classed by what is burning. An extinguisher is rated
for the classes it can handle, and using the wrong one ranges from useless to dangerous.
Most extinguishers on a wall are ABC dry chemical — one
unit covering the first three classes. Check the label; the classes it is rated for are printed
on it.
Metal fires, and what it takes to start one; Stop; Watch out
Metal fires, and what it takes to start one
Metal burns only when it is divided finely enough, and then only when several
conditions line up at once. Ordinary aluminum chips and swarf will not do this,
and neither will the quantities of fine material a lab space like this one generates. Solid stock
does not burn at all. The cases below are the ones that are genuinely different.
The form matters more than the metal
Magnesium is the real Class D case. Thin sections, chips and turnings
ignite readily and burn with intense heat and a brilliant white light, and dull tools alone can
produce enough heat during machining to start it.
Titanium turnings can ignite, and titanium fines and grinding dust are
worse — fine enough that a static discharge is a credible ignition source.
Aluminum fines — the dust off sanding, grinding, buffing and
polishing — are a genuine hazard, but only through the specific mechanisms below.
Aluminum chips and swarf are hard to ignite. Aluminum carries heat away
from a hot spot fast, it wears a tough oxide skin that holds together while the metal
underneath melts, and a chip has little surface area for its mass. Put a torch to a pile of
chips and they melt.
Solid stock does not burn. A block of aluminum is not fuel.
Magnesium and titanium are not common in student labs. A senior project
might bring one in. If you are about to cut, grind or sand either one, ask
first — every time.
Size is the usual line — shape is the exception
The line in the standard is about half a millimeter, measured across a
particle’s smallest dimension — which different editions write as
500 microns or as 420 microns (fine enough to pass a 40-mesh sieve), not two separate
limits. Below it, metal dust can carry an explosion. Above it, generally it cannot — and
generally is the word the standard uses, not never.
Flakes are the exception, and buffing and polishing make flakes. A flake is
wide but thin, so it is too big for the sieve and still burns like dust. Treat anything off a
buffing or polishing wheel as fines however big it looks. Machining chips are genuinely coarse
— that is the difference between a chip tray and a dust collector.
The ways fine metal actually ignites
A suspended dust cloud meeting an ignition source. Fines sitting in a tray
are not the hazard. Fines thrown into the air, at the right concentration, reaching a flame, a
torch, a spark or a static discharge, are — burning travels from one particle to the next
with extreme speed. It is why you never blow fine dust around, and why you do not raise a cloud
of it cleaning up.
Fines heavily mixed with rust or grinding scale. Aluminum plus iron
oxide — rust, or the scale off steel grinding — is a thermite reaction: the
aluminum strips the oxygen off the iron, so the mixture burns without needing air from outside.
That is what makes it a metal fire rather than an ordinary one, and why water and an ABC
extinguisher do nothing to it. It takes a real mixture to go — something near
three parts iron oxide to one part aluminum by weight, and an ignition source
far hotter than a spark. That is a rust-caked pile, not a trace. See Metal Chips and Swarf for how far
apart that threshold and the recycling one actually sit.
Wet fines. Aluminum fines in contact with water slowly give off hydrogen.
That is a reason not to seal damp fines into a closed container, and part of the reason water is
the wrong thing to put on a metal fire.
If fine metal does ignite
Do not fight it. Most general-purpose shops have no Class D
extinguisher — assume you do not have one unless somebody has shown you
where it is. Pull the alarm, get out, call 911, and tell the fire crew
it is a metal fire. That changes how they fight it, and they need to know
before they arrive with a hose.
PROHIBITED — the ABC extinguisher off the wall. “Dry
powder” (Class D) and “dry chemical” (ABC) are not the same thing. An ABC
unit throws an incompatible agent at pressure: it scatters burning fines and spreads the
fire.
NEVER put water on a metal fire. The stream throws burning material, can
raise an explosive dust cloud, and reacts with the metal to release hydrogen.
Alarm, evacuate, report.
Supporting detail: Addendum 13 — Why dry sand is on the list, and why it is probably not on yours.
What that means day to day
Do not let fine dust accumulate. Empty trays, vacuums and collectors rather than letting
them fill — see Machine Hazards and Housekeeping for housekeeping.
Chips and fines are disposed of differently, and the difference matters — see
Metal Chips and Swarf.
Let hot chips and debris cool before they go anywhere near a bin of paper or rag.
Ask before you machine an unfamiliar metal. If you do not know what it is,
that is the answer: ask.
Hot work and the things that start fires
Hot work and the things that start fires
Grinding throws sparks a surprising distance. Clear rag, sawdust, solvent
and packaging out of the area before you start, not after it smolders.
Oily rags — it depends entirely on which oil.Drying oils — linseed, tung, oil-based stains, varnishes and finishes
— cure by reacting with oxygen, and that reaction gives off heat. Bunched in a pile the
rags hold the heat in, and the pile can reach ignition on its own with nothing to light it.
Those rags NEVER go in a pile: spread them flat to dry, drop them in water, or
use the designated container.
Petroleum oils do not do that. Way oil, cutting fluid, hydraulic oil and
ordinary shop oil do not cure by oxidation, so a rag wiped with them will not self-heat and will
not spontaneously combust. It is still combustible — a spark or a hot
chip will light it like any oily cloth — so keep it away from hot work and out of a bin of
paper or sawdust. If you do not know which oil is on the rag, treat it as a drying
oil.
Chips come off hot, razor sharp and fast. How to handle them, how to clean them up, and the rules on compressed air.
Four reasons a chip is dangerous
Four reasons a chip is dangerous
A chip is not scrap until it has cooled and stopped moving. Straight off the
tool it is every one of these at once.
Hot
Where an aluminum chip forms, the cut runs roughly
250–650 °C (500–1200 °F), depending on the alloy
and the speed. Chips do not look it.
Sharp
The leading edge of a chip is always razor sharp. It is
a freshly cut edge and it will open a hand.
Strong
A long continuous chip is a steel ribbon. If it wraps a sleeve or a
limb it can pull you into the machine.
Slippery
Chips on the floor roll underfoot. This is one of the most common
ways people get hurt without the machine touching them.
Never clear chips with your hands; Stop
Never clear chips with your hands
Do not reach into a machine to clear chips while it is running, and do not
pick up a long stringy chip by hand at any time. Stop the spindle, then deal with it.
Gloves
Gloves may only be used for cleanup after the machine is shut
down.
Never wear gloves at a running machine. A glove catches where bare skin
would pull free, and takes your hand with it — see Machine Hazards and Housekeeping.
Brush
A brush may be used while the machine is in operation — your hands stay
outside the machine. If clearing the chip means reaching in, stop the spindle first.
On a CNC machine, take particular care: the tool can move without warning, and the
enclosure invites you to reach further in than you should.
Compressed air — there are limits on this; Watch out; Checklist
Compressed air — there are limits on this
Compressed air is convenient and it is the option people reach for first. It is also
regulated, because a chip in a moving air stream is a projectile and air
forced against skin can be driven into the body.
The rule
OSHA permits compressed air for cleaning only where it is
reduced to less than 30 psi, and only then with
effective chip guarding and personal protective equipment
(29 CFR 1910.242(b)). All three conditions, together — not the
pressure alone.
Chip guarding is anything that stops a chip reaching eyes or unbroken skin: a
protective cone nozzle covers the operator, and a screen or barrier is what covers everyone
else.
In practice
The 30 psi is measured at the nozzle, dead-ended — blocked by the
work or a hand — and is met by a limited air nozzle or a regulator, not by the supply
pressure upstream of it.
Eye protection, every time. Everyone nearby too — you do not get to decide the
range.
Never at skin, yours or anyone else’s.
Never toward another person, and check who is behind the machine first.
Never into an enclosed space.
If air would just relocate the mess into the air or across the shop, use a brush or the
vacuum instead.
Cleaning up; Stop; Checklist
Cleaning up
Use cleaning equipment or gloves to handle chips for disposal — the sharp edge does
not dull because the machine stopped.
Clear the machine so only the residue in the bottom tray remains.
Sweep the floor, and mop if the floor is wet with coolant.
If cleaning equipment such as a vacuum gets wet, open it up and let it dry
before it is put away.
Chips and fines do not go in the same place
Chips and swarf go in the recycling container. That container is for
chips only.
Fines go in the trash. Dust from sanding, grinding, buffing and polishing,
and what comes out of a dust collector — never the recycling container.
Why — two reasons, and the second one is the safety reason
The recycler pays for clean aluminum. A clean load gets the aluminum price;
mix another metal in and the whole load drops to a much cheaper one. Fines pick iron up —
off a shared belt or wheel, off steel work at the next bench — so fines do not go in.
Compare how often each container actually leaves the building. A chip
recycling container fills slowly and can stand most of a semester between pickups; the trash
goes out daily. Fines belong in the stream that leaves, not the one that stands in the corner
for months quietly collecting more of them. Anything whose problem is accumulation does
not go in the container designed to accumulate.
Two thresholds, same observation. “There is iron in the
fines” is a real problem for the recycling price and not a fire problem — and the
reason both are true at once is that the two thresholds are orders of magnitude apart. The price
threshold is a trace: a few steel chips are enough to drop the whole load to the
cheaper price. A thermite reaction needs iron oxide — rust or grinding
scale, not bright steel — at something near
three parts oxide to one part aluminum by weight, plus an ignition source far
hotter than a spark. That is most of the pile, not a trace. Most rules in a shop have a number
behind them; knowing which number you are being measured against, and how far you
actually are from it, is the difference between following a rule and understanding it.
Fine dust burns; chips do not. Aluminum chips and swarf are hard to ignite.
The fire hazard is fines — and then only when a cloud of them is thrown
into the air and meets an ignition source, or when a great deal of rust or steel grinding scale
is mixed into them. Do not let fine dust accumulate, and do not raise a cloud of it
cleaning up.
If fine metal debris does ignite, do not fight it. The ABC extinguisher on
the wall is the wrong tool and will scatter it. Alarm, evacuate, and tell the fire crew it is a
metal fire. See Fire Safety.
Safety/Universal Rules
Lab Conduct and Emergencies
What is never acceptable in a lab, what alertness actually requires, and what to do when something goes wrong.
Prohibited behavior; Stop
Prohibited behavior
NEVER operate equipment under the influence of drugs, alcohol, or medication that causes drowsiness.
NO horseplay, pranks or roughhousing in any lab area.
Do not distract others who are operating equipment.
No unauthorized experiments or modifications to equipment.
Staying alert
Staying alert
Stay focused — maintain concentration while operating equipment.
Take breaks when tired or distracted.
Ask questions if you are unsure about any procedure.
Report unsafe conditions immediately to the instructor.
Emergency procedures; Checklist
Emergency procedures
Know the location of emergency stops, fire extinguishers, first aid kits and exits.
Call 911 for serious injuries or fires.
Notify the instructor immediately of any incident, injury, or near-miss.
Do not move a seriously injured person unless they are in immediate danger.
For electrical shock specifically, the first action is different — see
If someone is shocked.
Workspace responsibility
Workspace responsibility
Clean as you go — do not wait until the end.
Report equipment problems before they become safety hazards.
Lab Conduct and Emergencies
Lean and Quality/Lean and Organization
5S Workplace Organization
The five-step workplace organization method. It is a lean manufacturing practice, and it is also why a tidy shop is a safer one.
Why 5S sits in a safety module
Why 5S sits in a safety module
5S is a lean manufacturing method for organizing a workplace. It
earns its place here because most of what it asks for is also what keeps people from getting hurt.
A cluttered bench hides a hazard. An unlabeled container is an unknown chemical. A floor with
chips on it is a slip. Every one of those is a 5S failure before it is an incident — which is
why the shutdown steps in After operating any equipment are 5S in
everything but name.
This page is the basics. 5S will get its own expanded treatment later.
Sort — Seiri
Sort — Seiri
Separate necessary items from unnecessary ones.
Remove or relocate items that do not belong in the work area.
Keep only what you need for the task in front of you.
Set in Order — Seiton
Set in Order — Seiton
Organize and label the remaining items clearly, for easy identification.
A place for everything, and everything in its place.
Create logical, efficient storage systems.
Shine — Seiso
Shine — Seiso
Clean work areas to maintain high hygiene standards.
Reduce accident risk through cleanliness and organization.
Inspect while cleaning — that is how problems get found early.
Establish consistent procedures for maintaining the first three S’s.
Create habits through regular practice and routine.
Ensure everyone follows the same organizational systems.
Sustain — Shitsuke
Sustain — Shitsuke
Continuously review and maintain all 5S practices.
Build the discipline to follow established procedures long-term.
Regular audits, and improvements to the system itself.
Engineering Fundamentals/Units and Measurement
Measurement Language
Use quantities, units, symbols, and SI prefixes precisely before a drawing, program, or calculation has a chance to drift.
A measurement is a number and a unit
A measurement is a number and a unit
A dimension on a drawing, a speed in a robot program, and a torque setting are all
quantities: a number paired with a unit. The number tells how many; the unit tells
what kind of thing and how large each part is.
25 mm
A length: twenty-five millimeters. Writing only 25 leaves
the measurement incomplete.
4.25 min
A CNC cycle time. It is not interchangeable with 4.25 seconds or
4.25 hours.
3.0 m/s
A speed or velocity magnitude. The slash means meters per
second.
Carry units through every line of a calculation. They are an error check,
not decoration. If the last line needs a length and the units say seconds, stop before the
wrong number reaches a drawing or controller.
Use the unit symbol exactly as specified: m for meter, s for
second, kg for kilogram. Symbols are not pluralized and do not take a period:
12 mm, not 12 mms.
Two systems you will encounter
Two systems you will encounter
The International System of Units (SI) is the standard system for science and
much technical work. U.S. drawings, hardware, materials, and equipment also use
U.S. customary units. Neither system lets us skip the unit; the job is to state
which one is being used and convert deliberately when they meet.
SI drawing25.0 mmmillimeters
U.S. customary drawing≈ 0.984 ininches
The part does not change. The measurement language does. A value
copied without its unit can make the same feature look like two different sizes.
SI base units used here
meter (m) for length, second
(s) for time, and kilogram (kg) for mass.
U.S. customary units used here
inch (in), foot (ft),
mile (mi), second (s), pound mass (lbm), and U.S.
liquid gallon (U.S. gal).
Coherent BG engineering system
The source slides call the coherent engineering
form BG (British Gravitational): foot, slug, and second. In that system,
slug · ft/s2 = lbf. A pound force and a pound mass are not the
same unit.
A gallon must be named. This unit set uses the U.S. liquid gallon
(U.S. gal), not an Imperial gallon.
Supporting detail: Addendum 14 — Why technical writing cares about the space.
SI prefixes change scale, not quantity
SI prefixes change scale, not quantity
A prefix is a power of ten attached to a unit. It makes a practical-sized number without
changing the physical quantity: 0.025 mm and 25 µm describe the same length.
Common engineering prefix ladderMove right: each unit is 1,000 times smaller, so the number is 1,000 times larger.
kilokm103 m
no prefixm100 m
millimm10−3 m
microµm10−6 m
nanonm10−9 m
1 m=1,000 mm=1,000,000 µm=1,000,000,000 nm
The ladder is a teaching subset; the complete reference follows. It shows why
1 mm = 0.001 m and 1 µm = 0.000001 m: changing a prefix changes the
number used to describe a length, not the length itself.
All current SI prefixes, plus the unprefixed unit used between them.
Name
Symbol
Factor
quetta
Q
1030
ronna
R
1027
yotta
Y
1024
zetta
Z
1021
exa
E
1018
peta
P
1015
tera
T
1012
giga
G
109
mega
M
106
kilo
k
103
hecto
h
102
deca
da
101
none
—
100
deci
d
10−1
centi
c
10−2
milli
m
10−3
micro
µ
10−6
nano
n
10−9
pico
p
10−12
femto
f
10−15
atto
a
10−18
zepto
z
10−21
yocto
y
10−24
ronto
r
10−27
quecto
q
10−30
Case matters.M is mega (106);
m is milli (10−3). A wrong capital letter changes a result by a
billion.
Prefix explorer
Prefix explorer
Choose two prefixes for the same base unit. The calculation compares their powers
of ten; it does not change what is being measured.
Move 3 powers toward larger units. The target unit
is 103 times larger, so the numerical value is divided by 103.
From: µm · 10^−6To: mm · 10^−3
smallest listed unit 10−30no prefix 100largest listed unit 1030
Result:
25 µm = 25 × 10−6 m = 0.025 ×
10−3 m = 0.025 mm.
Practice and sources; Practice
Practice and sources
Use the practice bank to apply this lesson’s prefix-conversion method.
Supporting detail: Addendum 15 — Sources and definitions.
Engineering Fundamentals/Units and Measurement
Dimensional Analysis
Convert quantities by multiplying by named equalities, cancelling units, and treating squared and cubed units as powers.
Convert by multiplying by one; Watch out
Convert by multiplying by one
A conversion factor is a ratio of two exactly equal physical quantities
written as a fraction. For example, 1 ft and 0.3048 m name exactly the same length. Their ratio
therefore has the numerical value 1, so multiplying by it changes the unit expression without
changing the physical quantity.
Either orientation is valid: 1 ft / 0.3048 m and
0.3048 m / 1 ft both equal 1. Choose the orientation that cancels the unwanted unit.
To convert 12 m to feet, put meters on the bottom:
12 m ×
1 ft0.3048 m
= 39.370078740… ft ≈ 39.3701 ft.
For the reverse conversion, turn the same exact equality over so feet cancel:
39.370078740… ft ×
0.3048 m1 ft
= 12 m.
Do not memorize an arrow. Write the desired unit, then arrange the factor so
the unwanted unit cancels. The units tell you whether the fraction is facing the correct way
before you calculate.
Exact, defined
1 in = 0.0254 m, so
1 ft = 0.3048 m and 1 yd = 0.9144 m exactly.
Keep guard digits
Use exact factors or sufficient digits while calculating;
round the displayed result only at the end and only as the task needs.
Match dimensions
Length converts to length, area to area, volume to volume,
and force to force. A calculator cannot make incompatible dimensions meaningful.
Powers apply to the whole conversion
Powers apply to the whole conversion
Area and volume are not lengths with decorative superscripts. The conversion factor itself
must be squared or cubed.
Why a single linear factor is not enough.
Quantity
Exact relationship
Useful result
Length
1 ft = 0.3048 m
1 ft = 0.3048 m
Area
(1 ft)2 = (0.3048 m)2
1 ft2 = 0.09290304 m2
Volume
(1 ft)3 = (0.3048 m)3
1 ft3 = 0.028316846592 m3
Time squared
(1 min)2 = (60 s)2
1 min2 = 3,600 s2
For example, 4 m2 × (1 ft / 0.3048 m)2 =
43.0556 ft2, which is sensibly reported as 43.1 ft2.
For liquid capacity, 1 m3 = 1,000 L and
1 U.S. gal = 3.785411784 L. The converter labels this as a U.S. liquid
gallon so it cannot be mistaken for an Imperial gallon.
Supporting detail: Addendum 16 — Dimensional analysis is also a design check.
Conversion bench
Conversion bench
This tool uses exact internal factors where standards define them. It only converts
within one quantity type; a length cannot become a speed without additional information.
Speed is a nonnegative magnitude and has no direction. A negative signed value
represents a velocity component opposite the chosen positive direction.
Result:
12 m × (1 ft / 0.3048 m) = 39.370078740… ft ≈ 39.3701 ft.
CNC production calculation
CNC production calculation
A CNC program estimates 4 min 15 s per part. The operator uses 30 min of an
8 h shift for setup. How many complete parts fit in the shift?
Convert the cycle: 4 min 15 s = 4.25 min.
Find machine-running time: 8 h × (60 min / 1 h) − 30 min = 450 min.
Divide running time by cycle time: 450 min / 4.25 min per part = 105.882....
105 complete parts. The fractional result is time into the
106th cycle, not a finished part. This assumes one machine, no unplanned stops, and that the
stated cycle time already includes every repeatable operation.
Supporting detail: Addendum 17 — Two more conversion cases from the unit.
Practice and sources; Practice
Practice and sources
Use the practice bank to apply cubic conversion factors to a model volume.
Supporting detail: Addendum 18 — Sources and exact factors.
Engineering Fundamentals/Motion and Rotation
Motion Quantities
Distinguish path length from displacement, and speed from velocity, before using time to describe a machine or vehicle in motion.
Path length and displacement answer different questions
Path length and displacement answer different questions
Distance is how much path was traveled. Displacement
is the directed change from the starting position to the ending position. A return trip can add
distance while leaving displacement at zero.
Distance
A nonnegative scalar path length. A conveyor that moves a tote 12 m
out and 12 m back travels 24 m of distance.
Displacement
A change in position with direction. If the tote returns to its
start, its displacement is 0 m even though it moved.
Coordinate choice
Choose a positive direction before calculating. Along a
straight robot rail, right might be positive and left negative.
Distance tells what the machine did along its path; displacement
tells where it ended up relative to where it began. Do not substitute one for the other
just because both use meters or feet.
Speed and velocity are not synonyms
Speed and velocity are not synonyms
Average speed is total distance divided by elapsed time. Average
velocity is displacement divided by elapsed time. Velocity includes direction; speed
does not.
average speed = total distance / elapsed time average velocity = displacement / elapsed time
Notation bridge: this site uses x for position
and Δx for displacement. Some course materials use s for position
instead. For a stated interval, write average velocity as
vavg = Δx / Δt; the symbols differ, but the physical idea is
the same.
For the 12 m out-and-back path completed in 16 s, average speed is
24 m / 16 s = 1.5 m/s. Average velocity is
0 m / 16 s = 0 m/s. Both statements can be true at the same time.
A production-line example
A mechanism must carry a part 12 m in 8 s. Its required average speed is
12 m / 8 s = 1.5 m/s. Converting with exact factors gives
1.5 m/s × (39.37007874 in / 1 m) = 59.055... in/s, or
59.1 in/s. If the programmed direction is stated, its average velocity is
+59.1 in/s in that direction.
Average and instantaneous readings
Average and instantaneous readings
An average uses a time interval. An instantaneous reading describes one moment: a car
speedometer reports instantaneous speed; a robot controller’s live velocity value is an
instantaneous velocity in its coordinate frame.
Use average speed for throughput, travel-time, and trip planning.
Use average velocity for a net movement over a stated interval.
Use an instantaneous reading when clearance, collision avoidance, or a
machine limit depends on what is happening now.
Supporting detail: Addendum 19 — The calculus idea, after the practical one.
Out-and-back path lab
Out-and-back path lab
Set positions along a straight path and the outbound and return times. The text
results make the distance and displacement distinction visible even when the track is not used.
−3 m15 m
Start: 0 mTurn: 12 mEnd: 0 m
Distance
Displacement
Average speed
Average velocity
Practice and sources; Practice
Practice and sources
Use the practice bank to apply distance, speed, and round-trip rate reasoning.
Calculate change in velocity over time, distinguish average from instantaneous acceleration, and convert squared time units correctly.
Acceleration is change in velocity over time
Acceleration is change in velocity over time
Acceleration is not simply “speeding up.” It is a change in velocity,
so it can describe speeding up, slowing down, or turning.
aavg = Δv / Δt = (vf − vi) / (tf − ti)
Δv
Change in velocity. With one chosen positive direction,
Δv = vf − vi.
m/s2
Meters per second per second. Each second, velocity changes
by the stated number of meters per second.
ft/s2
Feet per second per second. The coherent
foot–slug–second system uses this acceleration unit with slugs for mass.
Write the sign. A final velocity lower than the initial velocity produces
negative acceleration in the selected direction; it is not an error just because the answer is
negative.
Average is an interval; instantaneous is a moment
Average is an interval; instantaneous is a moment
Average acceleration is calculated over stated start and end conditions. An accelerometer or
control system can report instantaneous acceleration at one moment. They match at every moment only when the
acceleration stays constant through the interval.
Machine arm example
A machine arm starts from rest and reaches 3 m/s in 4 s:
aavg = (3 m/s − 0 m/s) / 4 s = 0.75 m/s2.
This is the average acceleration for the four-second move. If the drive ramps gently at the
start and end, its instantaneous acceleration changes during the move even though the average
remains 0.75 m/s2.
Robot gripper example
A SolidWorks motion study programs a gripper from 0 to 5 ft/s in 0.5 s to pick an electronic
component. Its average acceleration is 5 ft/s / 0.5 s = 10 ft/s2. In SI,
10 ft/s2 × (0.3048 m / 1 ft) = 3.048 m/s2.
Squared time needs a squared factor; Watch out
Squared time needs a squared factor
Acceleration has time in the denominator twice. When converting an acceleration unit, convert
the entire squared time relationship, not just one s.
1 min = 60 s means 1 min2 = (60 s)2 = 3,600 s2.
Use the inverse relationship in the correct direction.1 ft/s2 = 0.3048 m/s2, not
0.30482 m/s2. The foot is the only unit being changed in
that expression; seconds are already seconds in both units.
By contrast, converting m/min2 to m/s2
requires the full squared time factor. The unit cancellation shows why:
1 m/min2 × (1 min / 60 s)2 = 1/3,600 m/s2.
Acceleration lab
Acceleration lab
Change the initial and final velocities and the elapsed time. The last result
converts the calculated foot-per-second-squared value to SI.
Change in velocity
Average acceleration
SI equivalent
Practice and sources; Practice
Practice and sources
Use the practice bank to apply average acceleration over a stated interval.
Scale CAD geometry correctly, connect volume and density to mass, and keep force and weight as separate quantities.
Scale changes area and volume by powers; Watch out
Scale changes area and volume by powers
If every linear dimension of a model is multiplied by a scale factor s,
area changes by s2 and volume changes by s3. A
20% larger model is not 20% larger in area or volume.
Length
Lnew = sLold
Area
Anew = s2Aold
Volume
Vnew = s3Vold
For s = 1.2, area factor = 1.22 = 1.44 and volume factor
= 1.23 = 1.728. This is why a modest scale change can matter to material
use, shipping mass, tank capacity, and actuator selection.
Never scale an area with a linear factor or a volume with an area
factor. The exponent belongs to the geometry, not to the number of decimal places.
Volume is capacity only after you name the unit
Volume is capacity only after you name the unit
CAD mass properties often report volume in a model’s document units. Before treating that
number as a tank capacity or a material quantity, state the volume unit and convert it to the
form the drawing or specification requires.
Volume relationships used in this unit.
Relationship
Meaning
1 m3 = 1,000 L
A cubic meter contains one thousand liters.
1 U.S. gal = 3.785411784 L
This is a U.S. liquid gallon, not an Imperial gallon.
1 ft3 = 7.48051948 U.S. gal
Derived from the exact foot and U.S. gallon definitions.
Static solved reservoir example
A SolidWorks model gives a hydraulic reservoir internal volume of 2.5 ft3. Its
capacity is 2.5 ft3 × 7.48051948 U.S. gal/ft3 =
18.7013 U.S. gal, or 18.7 U.S. gal. This assumes the reported CAD volume
is the usable internal volume and no design headspace has yet been subtracted.
Density connects volume to mass
Density connects volume to mass
Density is mass per volume, and its symbol is ρ (rho):
ρ = m/V. Turned around, when material density and CAD volume use compatible
units, m = ρV produces mass.
(kg/m3) × (m3) = kg
Density units in the two systems.
System
Unit
Conversion
SI
kg/m3
1 kg/m3 = 0.00194032 slug/ft3
Foot–slug–second
slug/ft3
1 slug/ft3 = 515.3788 kg/m3
For example, a volume of 0.13824 m3 made of material with a density of
2,700 kg/m3 has mass
m = 2,700 kg/m3 × 0.13824 m3 = 373.248 kg.
Static solved steel example
A steel I-beam has a volume of 0.2 m3 and a density of 7,850 kg/m3. Its
mass is m = 7,850 kg/m3 × 0.2 m3 = 1,570 kg. That is the
same mass the weight example below starts from — a CAD volume and a material card are
usually where a weight calculation actually begins.
Mass does not change merely because an object is moved from one
planet to another. Weight can change because gravitational acceleration changes. CAD
models, material databases, and shipping specifications commonly need mass; lifting and support
calculations commonly need force or weight.
Supporting detail: Addendum 22 — Check the CAD assumptions before trusting mass properties.
Force and weight are separate quantities
Force and weight are separate quantities
Force is a push or pull. For constant mass, Newton’s second law is
Fnet = ma. Weight is one particular force: the force due
to gravity, written W = mg.
Fnet
Net force, in newtons (N) or pound force
(lbf). It is the combined force that produces acceleration.
W
Weight, a gravitational force. Near Earth’s standard gravity,
g0 = 9.80665 m/s2; local gravity can differ slightly.
m
Mass, in kilograms, pound mass, or slugs. It is not measured in newtons or
pound force.
In coherent SI, 1 N = 1 kg · m/s2. In the coherent
foot–slug–second system, 1 lbf = 1 slug · ft/s2. Do not
silently replace lbm with lbf.
Static solved weight example
For a 1,570 kg mass at standard gravity, W = mg = 1,570 kg ×
9.80665 m/s2 = 15,396.44 N, or 15.4 kN. This is a weight
calculation at standard gravity, not a claim that the mass is 15.4 kN.
CAD scale, mass, and weight lab
CAD scale, mass, and weight lab
This model begins with an area and volume in SI units, scales them, then uses
density and gravitational acceleration to show the separate mass and weight results.
Area factor
Volume factor
Scaled area
Scaled volume
Mass
Weight force (N)
Weight force (lbf)
Practice and sources; Practice
Practice and sources
Use the practice bank to apply squared-area conversion and complete-count reasoning.
Supporting detail: Addendum 23 — Sources and engineering context.
Engineering Fundamentals/Motion and Rotation
Angular Motion
Measure rotation in degrees, radians, and revolutions, then use angular velocity and angular acceleration to describe a turning shaft.
Rotation is measured three ways
Rotation is measured three ways
Angular displacement is how far something has turned. Its symbol is
θ (theta), and there are three units in everyday use for it. They measure
the same rotation; they differ only in how much turning counts as one unit.
Revolution (r)
One complete turn. This is what a machine nameplate counts.
Degree (°)
One revolution cut into 360 parts. This is what a drawing and a
protractor use.
Radian (rad)
The angle whose arc is exactly as long as the radius. This is the
SI unit, and it is the one formulas such as v = ωr expect.
A radian is defined by the circle itself, not by a count somebody picked. Swing the
radius around the rim until the arc it traces is as long as the radius, and the angle you have
opened is one radian.
The three units, describing one and the same rotation.
In revolutions
In degrees
In radians
1 r
360°
2π rad = 6.283185 rad
0.5 r
180°
π rad = 3.141593 rad
0.25 r
90°
π/2 rad = 1.570796 rad
≈ 0.159 r
≈ 57.29578°
1 rad
The two factors worth keeping to hand: 1° = 0.01745329 rad and
1 rad = 180°/π = 57.29578°.
The degree sign sits tight against the number —
90°, not 90 °. Every other unit symbol takes a space:
1.57 rad, 45 r/min. The degree, minute, and second of plane angle are
the only exceptions to that rule.
Supporting detail: Addendum 24 — Why a radian is barely a unit at all.
Angular velocity is how fast it turns; Watch out
Angular velocity is how fast it turns
Angular velocity uses the symbol ω (omega), and it is
directed angle change per time interval for rotation about a fixed axis:
ωavg = Δθ / Δt. Instantaneous angular
velocity is the rate at one moment; it equals this average throughout the interval only for
constant angular velocity.
Supporting detail: Addendum 25 — Where 0.1047198 comes from.
Angular acceleration is how fast the turning changes
Angular acceleration is how fast the turning changes
Angular acceleration uses the symbol α (alpha), and it
is change in angular velocity divided by the time it took:
αavg = Δω / Δt
Its SI unit is rad/s2. Everything true of straight-line acceleration on
Acceleration and Squared Time is true here as well: it is a change, so a shaft
slowing down has angular acceleration opposite its angular velocity (negative if it is turning
in the positive direction), and
the squared second means a squared factor whenever the time unit changes.
Worked example: a motor speeding up
A motor shaft is turning at 17 rpm. Power to the motor is increased, and 1.1 s later it is
turning 8 rpm faster. What is the angular acceleration in rad/s2?
Only the change matters, so convert the 8 rpm increase:
8 r/min × 0.1047198 rad/s per r/min = 0.837758 rad/s.
Divide by the time: 0.837758 rad/s ÷ 1.1 s = 0.7616 rad/s2.
0.76 rad/s2, as an average over those 1.1 s. The
starting 17 rpm never enters the calculation — acceleration is built out of the change, not
out of the speed.
Worked example: a spindle running up
A machining-centre spindle goes from rest to 8,000 rpm in 2.5 s.
8,000 r/min × 0.1047198 rad/s per r/min = 837.758 rad/s.
That is the average over the run-up. A drive that ramps gently at each end has
a changing instantaneous angular acceleration inside the same interval, exactly as a linear drive
does.
Sources
Sources
Supporting detail: Addendum 26 — Where these values were checked.
Engineering Fundamentals/Motion and Rotation
Rotation and Linear Speed
Turn a shaft speed into the speed of what it drives, and back again, using the radius - belts, rollers, wheels, and grinding wheels.
The radius is what links turning to travelling; Watch out
The radius is what links turning to travelling
A roller turns; the belt on it travels. A wheel turns; the vehicle moves. The two
speeds are not the same number, and the thing that converts one into the other is the
radius.
v = ωr · a = αr
Here a is the tangential acceleration, not the rim point’s total
acceleration: it also has an inward component ω2r. Belt and
vehicle speeds match rim speed only when there is no slipping.
v
The straight-line speed of a point on the rim — the speed of the belt,
the sheet, the vehicle.
ω
Angular velocity, in radians per second. See
Angular Motion for the conversion from rpm.
r
The radius, in the same length unit you want the answer in.
Rollers and wheels are almost always specified by diameter, so halve it first.
Both of these formulas are only true when the angle is in radians. Feed
them rpm and the answer is wrong by a factor of about 9.55; feed them degrees per second and it
is wrong by a factor of about 57.3. Convert to rad/s first, every time.
Two mistakes account for nearly every wrong answer here: using the diameter where
the radius belongs, and leaving the speed in rpm. Both are worth a deliberate check before the
arithmetic starts.
Supporting detail: Addendum 27 — Why the radian is the only angle unit that works.
Worked example: a conveyor drive roller
Worked example: a conveyor drive roller
A conveyor belt runs over a drive roller 200 mm in diameter, turning at 45 rpm. What is the
belt speed, and how long does a package take to travel 15 m?
Halve the diameter: r = 100 mm = 0.100 m.
Convert the speed: 45 r/min × 0.1047198 rad/s per r/min = 4.712389 rad/s.
Multiply: v = 4.712389 rad/s × 0.100 m = 0.4712 m/s.
Divide the distance by the speed:
15 m ÷ 0.4712389 m/s = 31.83 s.
0.47 m/s, and about 32 s for 15 m. That assumes the belt
does not slip on the roller, which is the assumption a real drive is designed to make true.
Worked example: a roll-forming feed rate
Worked example: a roll-forming feed rate
Forming rolls 150 mm in diameter rotate at 25 rpm. What is the feed rate of the sheet in
m/min, and how long does 20 m of sheet take?
r = 75 mm = 0.075 m.
25 r/min × 0.1047198 rad/s per r/min = 2.617994 rad/s.
v = 2.617994 rad/s × 0.075 m = 0.19635 m/s.
The question asks for metres per minute, so convert the time unit:
0.19635 m/s × 60 s/min = 11.78 m/min.
20 m ÷ 11.78 m/min = 1.70 min, which is about 1 min 42 s.
Note what step 4 did and did not do. Changing seconds to minutes in a speed takes one
factor of 60. If the quantity had been an acceleration, the same change would take
602 — see Acceleration and Squared Time.
Worked example: running the conversion backwards
Worked example: running the conversion backwards
Sometimes the linear quantity is what you know. The formulas simply rearrange:
ω = v/r and α = a/r.
A wheel, from angular to linear
A tyre 28 in in diameter turns at 3.5 rad/s. How fast is the vehicle moving, in miles per hour?
r = 14 in × 0.0254 m/in = 0.3556 m.
v = 3.5 rad/s × 0.3556 m = 1.2446 m/s.
1.2446 m/s ÷ 0.44704 m/s per mph = 2.78 mph.
A wheel, from linear to angular
A vehicle accelerates at 5 m/s2 on tyres 78 cm in diameter. What is the angular
acceleration of a wheel?
r = 39 cm = 0.39 m.
α = 5 m/s2 ÷ 0.39 m = 12.8 rad/s2.
Check the unit on the answer, not just the number. Dividing
m/s2 by m leaves 1/s2, and because
the radian is a ratio of two lengths, rad/s2 is the same thing named for
what it describes.
Rim speed is why wheel size changes the safe rpm; Stop
Rim speed is why wheel size changes the safe rpm
A grinding wheel is limited by how fast its rim moves, not by how fast its centre
turns. Put a bigger wheel on the same spindle at the same rpm and the rim goes faster, because
every point on it travels a longer circle in the same time.
Take a wheel whose rim speed must stay at or below 35 m/s:
Same 35 m/s rim-speed limit, two wheel sizes.
Wheel diameter
Radius
ω = v/r
Same speed in rpm
200 mm
0.100 m
350 rad/s
3,342 rpm
250 mm
0.125 m
280 rad/s
2,674 rpm
The larger wheel has to run slower, by about 670 rpm, to keep the same rim
speed. Nothing about the machine changed; only the radius did.
Do not calculate your way to a grinding-wheel speed. The number that governs
is the maximum operating speed marked on the wheel, and OSHA requires that the
spindle speed of the machine be checked before a wheel is mounted, to be certain it
does not exceed that marking (29 CFR 1910.215(d)(1)). The arithmetic
above explains why a bigger wheel is marked slower. It does not authorise a wheel, and
it is not a substitute for reading the wheel. See Machine Hazards and Housekeeping.
Sources
Sources
Supporting detail: Addendum 28 — Where these values were checked.
Engineering Fundamentals/Force and Power
Torque
Turning effort is force times radius - how to calculate it, which unit belongs to it, and why the order of the two words is not decoration.
Torque is force applied at a radius; Watch out
Torque is force applied at a radius
A force pushes. A torque turns. The same force produces more
torque the further it acts from the axis of rotation, which is why a longer wrench loosens a
tighter nut with the same pull.
The force acts at right angles to the radius. Everything below assumes that; a force
pointing partly along the radius contributes only the part of it that is perpendicular.
r is the radius, measured from the axis of rotation to where the force acts.
Pulleys, rollers, and wheels are specified by diameter, so halve the number on the drawing
before it goes into this formula.
Note: when a turning effort is described about an axis rather
than about a shaft, it is often called a moment and given the symbol
M. It is the same calculation.
The unit, and the word order that identifies it
The unit, and the word order that identifies it
Torque units and rounded conversion factors between them.
System
Unit
Symbol
Conversion
SI
newton metre
N·m
1 N·m = 0.7375621 lbf·ft
Foot–slug–second
pound-force foot
lbf·ft
1 lbf·ft = 1.355818 N·m
Case matters, and this one bites. The SI torque unit is
N·m with a lower-case m. Written N·M it is not a valid SI torque unit: M is the
prefix for 106, but a prefix cannot stand alone as a unit. The same trap catches Kg for kg and S for
s. See Measurement Language.
Here torque is written lbf·ft; energy is written ft·lbf.
The same two units, the same numerical factor, written in the opposite order — and NIST
prints them that way round on purpose: pound-force foot converts to the newton metre, foot
pound-force converts to the joule. They are different physical quantities that happen to share
a unit combination. Word order is a convention, not a mathematical distinction; use the
quantity and context to tell them apart. SI avoids the ambiguity by giving energy its own name, the joule; a torque is never
written in joules. See Work and Energy.
Worked example: can the motor hold the arm up?
Worked example: can the motor hold the arm up?
A robot-arm joint motor produces 15 N·m. The arm segment is 0.35 m long and carries a
25 N load at its end. Will the motor hold the arm horizontal?
The load acts straight down, at right angles to a horizontal arm, at the full 0.35 m:
τ = 0.35 m × 25 N = 8.75 N·m.
Compare with what the motor produces:
8.75 N·m < 15 N·m.
Yes, with 6.25 N·m to spare — for the load
alone. The weight of the arm segment itself also produces a torque about the joint, and no
mass was given for it, so this answer is a partial one. In a real selection you would add the arm
weight acting at its own centre of mass, then keep margin on top of that.
This is the shape of most torque questions: work out what the load demands, then check it
against what the drive can supply, and be explicit about what you have left out.
Worked example: torque from a tangential force
Worked example: torque from a tangential force
A wheel 250 mm in diameter needs 3.5 kN of tangential force to overcome resistance. What torque
must the motor supply to the axle?
r = 125 mm = 0.125 m.
3.5 kN = 3,500 N.
τ = 0.125 m × 3,500 N = 437.5 N·m.
The same formula, rearranged
When the torque is what you know and the force is what you want,
F = τ/r. That single rearrangement explains a family of everyday machines: a
longer wrench, a bigger steering wheel, and a larger pulley all trade radius against force. Double
the radius and the same torque delivers half the force — and, at the same rotational speed,
the rim travels twice as far, which is why Power and Efficiency comes out unchanged.
Sources
Sources
Supporting detail: Addendum 29 — Where these values were checked.
Engineering Fundamentals/Motion and Rotation
Gear Ratios
Follow tooth counts through pairs, idlers and compound trains; multiply stage efficiencies and choose gears to meet speed and torque limits.
Experiment: trade speed for turning effort; Interactive
Experiment: trade speed for turning effort
Predict first: a 20-tooth gear turns at 120 rpm clockwise and drives a 40-tooth gear. Will the larger gear turn faster or slower? What changes if you add an idler between them?
One mesh: 2:1 reduction
B has 2× as many teeth as A. Each passing tooth advances B by one tooth space; B turns 0.5× as fast, in the opposite direction. At 120 rpm clockwise and 2 N·m input, output B is 60 rpm CCW and 4 N·m ideally. The dashed circles are pitch circles, where the speeds match.
Add an idler: still 2:1
The idler changes direction twice: A → I → B. Its 30 teeth cancel from (30 ÷ 20) × (40 ÷ 30). At 120 rpm clockwise and 2 N·m input, output B is 60 rpm CW and 4 N·m ideally. The dashed circles are pitch circles, where the speeds match.
Two stages: 2 × 2 = 4:1
B and C turn together. Multiply the two reductions: (40 ÷ 20) × (40 ÷ 20) = 4. At 120 rpm clockwise and 2 N·m input, output D is 30 rpm CW and 8 N·m ideally. The two front-view meshes are separated on the page; the dashed connector represents their common shaft.
All three examples use the same ideal input: 120 rpm and 2 N·m. Input power is 25.13 W, and ideal output power is also 25.13 W. More output torque comes with less speed.
With each actual mesh at 96% efficiency, the pair delivers 3.84 N·m and 24.13 W; the idler train delivers 3.6864 N·m and 23.16 W; the compound train delivers 7.3728 N·m and 23.16 W. Their output speeds remain 60, 60 and 30 rpm. This comparison charges a loss at both idler meshes.
Count the teeth to find the speed
Count the teeth to find the speed
The driver supplies motion; the driven gear receives it. For one external gear mesh, each tooth passing on the driver advances the driven gear by one tooth space. A gear with twice as many teeth needs twice as many passing teeth to complete a turn.
This lesson uses reduction ratio i = input speed ÷ output speed, with speed magnitudes. A 2:1 reduction means two input turns for one output turn. Ratios above 1 reduce speed; ratios below 1 increase it. At zero speed, use tooth counts to find the ratio; do not divide 0 by 0.
Notation map: this page's original equations use N for teeth and n for speed. The course uses n for teeth, ω for angular velocity and τ for torque. Thus page N = course n; page speed n is written ω in the additions below. GR and i name the same reduction ratio.
In course notation, using magnitudes: GR = nout/nin = dout/din = ωin/ωout = τout/τin for an ideal single pair. Here d is pitch diameter; the torque equality assumes no losses. For a compound train, multiply the stage ratios; the first and last tooth counts alone do not give the overall ratio.
Supporting detail: Addendum 30 — Why tooth counts work, and what the dashed circles mean.
An idler and a compound shaft do different jobs
An idler and a compound shaft do different jobs
One mesh reverses
A → B turns the output opposite to the input, viewed from the same end of each shaft.
An idler cancels
A → I → B reverses twice. I affects its own speed and the spacing, but its tooth count cancels from the end-to-end ratio.
Compound stages multiply
A → B, then C → D, with B and C fixed together: i = (NB/NA) × (ND/NC).
Same shaft means the same angular speed. A large B and a small C fixed to one shaft make the same number of turns in the same direction. Their rim speeds differ because their radii differ. They do not mesh with each other.
In the compound example, 20 → 40 teeth halves the speed. A second 20 → 40 stage halves it again: 120 → 60 → 30 rpm. The two external meshes make the final output turn in the same direction as the input.
An idler is not another reduction stage. Drop its tooth count when finding the end-to-end ratio, but count every external mesh for direction: odd means opposite; even means the same, viewed from the same end of the parallel shafts. Do not drop a gear that shares a shaft with a different gear in a compound train.
More torque costs speed; it does not create power
More torque costs speed; it does not create power
Torque is turning effort. In this ideal, lossless train at steady load, output torque magnitude = input torque magnitude × reduction ratio. A 2:1 reduction changes 120 rpm and 2 N·m into 60 rpm and 4 N·m. The 4:1 compound example gives 30 rpm and 8 N·m.
Rotational power is torque × angular speed: P = T × 2πn/60 when T is in N·m and n is in rpm. Both sides of either example carry 25.13 W ideally. Real friction and other losses leave less output power. Tooth strength, bearings, shafts, lubrication and the motor all limit usable torque.
At zero speed, mechanical power is zero. A loaded, stationary gear train can still carry torque. The lab shows ideal static torque balance in that case; it does not model motor stall behavior or promise a safe load.
Supporting detail: Addendum 31 — Primary references and model boundaries.
Each stage receives only the power that survived the stage before it. Use decimal efficiencies and multiply: ηtotal = η1 × η2 × η3. Never add or average them. See Power and Efficiency for the general meaning of efficiency.
Power-flow schematic, with gear pairs shown by pitch circles. The stages are separated for clarity; each connecting shaft turns its attached gears together.
At 98% per stage, three stages give 0.98³ = 0.941192: about 5.88% total loss, not 6%. Fewer, higher-quality stages often beat many cheap stages for efficiency, provided they can meet the ratio and load requirements.
Supporting detail: Addendum 32 — Why adding losses is only an approximation.
Positive drives keep the speed ratio; losses reduce torque
Positive drives keep the speed ratio; losses reduce torque
A positive drive keeps input and output linked in a fixed ratio without slipping. Gears, chains and timing belts are positive drives. A slipping flat belt or V-belt is not. Follow Rotation and Linear Speed for the connection from rotation to belt travel.
At a stated steady input speed and load, use magnitudes:
ωout = ωin/i τout = τin × i × ηtotal Pout = ηtotal × Pin
The teeth still set the speed exactly in this model. Efficiency reduces output torque from its ideal value. It does not reduce output rpm as well. Use matching torque units on both sides: lbf·ft or N·m. The course conversion is 1 rpm ≈ 0.1047 rad/s when angular speed in rad/s is needed.
Supporting detail: Addendum 33 — Follow both stages of one loaded train.
Count stages for ratio, meshes for direction and stated losses
Count stages for ratio, meshes for direction and stated losses
For a simple train A → I → B, the idler cancels from (NI/NA) × (NB/NI) = NB/NA. The two external meshes still reverse direction twice.
Follow the loss assumption in the problem. Real meshes lose some power, but a problem may explicitly ignore it. If every actual mesh is 96% efficient, A → I → B has ηtotal = 0.96². If a whole stage including its idler is assigned 96%, use that stage value once. If η = 1.00 is stated, ignore losses. Do not infer the loss count from the reduction-stage count when an idler is present.
Choose teeth, then check both output limits; Checklist; Practice
Choose teeth, then check both output limits
Record input speed and torque, the output speed ceiling and torque floor, available integer tooth counts, maximum ratio per stage, and the loss assumption.
Use the speed ceiling to find i ≥ ωin/ωceiling. With at most R:1 per stage, k reduction stages can provide at most Rk:1.
For each candidate stage count k, calculate ηtotal and check the torque bound i ≥ τfloor/(τin × ηtotal). Use the larger of the speed and torque bounds.
Choose whole-tooth pairs within the range and per-stage limit. Connect successive pairs by shared shafts. Multiply their actual ratios; do not assume a rounded target is achievable.
Calculate output speed and torque, keeping full precision for both limit checks. Check direction by counting external meshes. An added idler may require recalculating losses.
To choose the faster of feasible designs at the same input speed, compare their actual overall ratios: the smaller one is faster. A feasible design is not automatically the fastest possible design.
Supporting detail: Addendum 34 — Worked design: a winch with a speed ceiling and torque floor.
Force moving through a distance is work - the joule, the foot pound-force, and why an energy unit reads backwards from a torque unit.
Work is a force moving something through a distance
Work is a force moving something through a distance
Holding a heavy box still is exhausting, and in this sense it is zero work. Work
needs a component of force along the displacement; work is negative when that component
opposes the movement.
W = Fs — work equals force times displacement for a constant force parallel to the motion.
Work is one of the ways energy moves from one place to another, so it is measured in energy
units and is often written E when what matters is the energy delivered rather than
the act of delivering it.
The two systems, for work and every other form of energy.
System
Unit
Symbol
Built from
SI
joule
J
1 J = 1 N·m
Foot–slug–second
foot pound-force
ft·lbf
1 ft·lbf = 1.355818 J
Worked example: lifting a load
How much work is required to lift a 2,000 lb load to a height of 10 ft?
The force needed to lift steadily is the load’s weight, 2,000 lbf, and it acts
straight up along the 10 ft of travel.
W = 2,000 lbf × 10 ft = 20,000 ft·lbf.
In SI: 20,000 ft·lbf × 1.355818 J per ft·lbf = 27,116 J, or
27.1 kJ.
Two things this calculation assumes, both worth saying out loud: the load is
raised at a steady speed, so no extra force goes into accelerating it, and the 2,000 lb figure is
a weight in pound-force, not a mass in pound-mass. On
Geometry, Mass, and Force those are separate quantities, and here it is the force that belongs
in the formula.
Work and torque share dimensions - word order is a convention; Watch out
Work and torque share dimensions - word order is a convention
Multiply a constant force by displacement along that force and you get work. Multiply a force by a radius and you get
torque. Both are a force times a length, so in the foot–pound system both come out as some
arrangement of feet and pounds-force.
Here torque is written lbf·ft. Energy is written
ft·lbf. The numerical factor is identical — 1.355818 of
either — but word order alone does not establish the physical quantity. Torque describes turning
effort; work describes energy transferred through displacement.
SI removes the ambiguity by naming the energy unit separately. A torque stays
N·m; energy becomes the joule. Numerically
1 J = 1 N·m, but a torque is never reported in joules. See Torque.
Supporting detail: Addendum 35 — Turning a torque into work, and where the radian goes.
The energy units you will actually meet
The energy units you will actually meet
Energy is billed, rated, and specified in a lot of different units. They all convert; the only
work is knowing which one a number is in.
Common energy units, expressed in joules.
Unit
Symbol
In joules
Where it turns up
joule
J
1 J
The SI unit. Everything else converts to it.
foot pound-force
ft·lbf
1.355818 J
U.S. mechanical work and energy.
watt hour
W·h
3,600 J (exact)
Battery capacity.
kilowatt hour
kW·h
3,600,000 J (exact)
The line on an electricity bill.
British thermal unit (IT)
BtuIT
1,055.056 J
Heating, cooling, and fuel ratings.
horsepower hour
hp·h
≈ 2,684,520 J
Engine and drive energy.
calorie (IT)
calIT
4.1868 J (exact)
Thermal work and material data.
A kilowatt hour is a power multiplied by a time, and that is all it is. One
kilowatt sustained for one hour. It is not an SI unit — NIST lists it among the units to
be converted into SI — but it is exactly 3.6 MJ, and it is the unit an electricity
meter counts in.
“Btu” on its own is ambiguous. NIST lists six
different British thermal units, from 1,054.35 J to 1,059.67 J depending on which definition is
meant. The spread is about half a percent, which is small until it is multiplied by a fuel bill.
Use BtuIT unless a specification names another one.
Sources
Sources
Supporting detail: Addendum 36 — Where these values were checked.
Engineering Fundamentals/Force and Power
Power and Efficiency
Power is work per unit time - three equivalent ways to calculate it, the horsepower conversions, and what an efficiency figure can and cannot be.
Power is how fast work gets done
Power is how fast work gets done
Two hoists that lift the same load to the same height do the same
work. The one that does it in half the time needs twice the power.
P = W / t — average power equals work divided by elapsed time.
The two power units and the factors between them.
System
Unit
Symbol
Definition and conversion
SI
watt
W
1 W = 1 J/s; 1 W = 0.001341022 hp
Foot–slug–second
horsepower
hp
1 hp = 550 ft·lbf/s; 1 hp = 745.6999 W
The symbol W does double duty: upright W after a number
is the watt, while W standing in a formula for a quantity is usually work. Context
separates them: P = W/t uses W for work, while
1 W = 1 J/s uses it for the watt.
Worked example: powering the lift
On Work and Energy, lifting 2,000 lbf through 10 ft took 20,000 ft·lbf, or 27.1 kJ.
How much power does doing it in 4 s require?
In U.S. units: 20,000 ft·lbf ÷ 4 s = 5,000 ft·lbf/s, and
5,000 ÷ 550 = 9.09 hp.
In SI: 27,116 J ÷ 4 s = 6,779 W, or 6.78 kW.
Cross-check the two: 9.0909 hp × 745.6999 W/hp = 6,779 W. They agree,
which is the point of doing both.
That is the power delivered to the load. A motor sized for this job needs more than that,
because no drive is perfectly efficient.
The same power, three ways to reach it; Watch out
The same power, three ways to reach it
Which form you use depends on what you have been given, not on which is more correct. All three
produce watts in SI. In P = Fv, force and velocity must be parallel;
otherwise use the force component along the velocity.
Three routes to a power, in each system.
Form
SI
Foot–pound
Work over time P = W/t
J/s = W
(ft·lbf/s) ÷ 550 = hp
Force times speed P = Fv
N × (m/s) = W
(lbf × ft/s) ÷ 550 = hp
Torque times angular velocity P = τω
(N·m) × (rad/s) = W
(lbf·ft × rad/s) ÷ 550 = hp
In the third form the angular velocity must be in rad/s. An rpm figure
substituted directly is wrong by a factor of about 9.55. Convert it first —
Angular Motion.
The divisor 550 is not a fudge factor. One horsepower is defined as 550 pound-force
feet of work per second, so dividing by 550 is simply converting the unit.
Two shortcut formulas, and the conditions attached to them
Two shortcut formulas, and the conditions attached to them
These two save a lot of arithmetic in practice. Both are unit conversions with an assumption
hidden inside.
From volts and amps
hp = (volts × amps) ÷ 746
The 746 is exact: NIST defines a separate unit, horsepower (electric), as 746 W. So
the formula is really two steps — find the electrical power in watts, then convert watts to
horsepower.
The hidden condition is in the first step. Volts times amps gives real power
in watts for a direct-current circuit or a purely resistive load. For single-phase AC, RMS volts times RMS amps
gives apparent power, in volt-amperes; the real power in watts is that multiplied by
the power factor, the ratio of real power to apparent power. Use the shortcut
on an AC motor without its power factor and the answer comes out high. See
Current, Voltage, and Resistance.
From torque and rpm
hp = (torque in lbf·in × speed in rpm) ÷ 63,025
This one is the P = τω row above, with the rpm-to-rad/s conversion and
the inch-to-foot conversion already folded into the constant. It only works with the torque in
pound-force inches and the speed in rpm; feed it
lbf·ft and the answer is twelve times too small.
Supporting detail: Addendum 37 — Where 63,025 comes from.
Efficiency is the fraction that makes it through; Watch out
Efficiency is the fraction that makes it through
The efficiency of a machine is the ratio of useful output to total input. Its
symbol is η (eta), and it can be written with either power or work as long as
both sides of the ratio use the same one:
η = Pout / Pin ·
η = Wout / Win
It is a ratio of two like quantities, so the units cancel: efficiency is a plain number, usually
quoted as a percentage.
For a real machine in steady operation, η < 1; the ideal lossless limit is 1. You cannot get more power out than you
put in, and some of every input always leaves as heat, noise, or friction rather than as useful
output. A calculated efficiency above 1 means an error in the numbers, not a remarkable
machine.
Worked example: an electric hoist motor
A motor consumes 500 W and applies 1,000 N of force to lift an object at 0.45 m/s. What is the
efficiency of the system?
Useful output, using P = Fv:
1,000 N × 0.45 m/s = 450 W.
η = 450 W ÷ 500 W = 0.90, or 90%.
The missing 50 W has not vanished. It is power lost rather than delivered to the load, typically as heat in the motor and drive.
Worked example: follow power through two stages
A hypothetical steady system receives 100 W. Stage 1 is given as 80% efficient, and Stage 2
is given as 90% efficient. Each percentage applies to the power entering that stage.
Useful power continues across the top. Each loss branches at the boundary where it occurs.
Stage 1 output: 100 W × 0.80 = 80 W. Stage 1 loss:
100 W − 80 W = 20 W.
Stage 2 receives 80 W, not the original 100 W. Its output is
80 W × 0.90 = 72 W. Its loss is 80 W − 72 W = 8 W.
Overall efficiency: 72 W / 100 W = 0.72, or 72%. Equivalently,
0.80 × 0.90 = 0.72.
Total accounted loss: 20 W + 8 W = 28 W. Check the boundary:
72 W useful + 28 W loss = 100 W input.
Do not add 20% + 10% and call the system 70% efficient. The 20% loss is
measured from 100 W, while the 10% loss is measured from the 80 W that reaches Stage 2. Watts may be added here
because 20 W and 8 W are amounts of power accounted across the same overall boundary.
Work backward when the required output is known: Stage 2 needs 72 W / 0.90 = 80 W at its input,
and Stage 1 needs 80 W / 0.80 = 100 W. The same result comes from
72 W / 0.72 = 100 W. Use Gear Ratios to explore the same multiplication idea for
stated per-mesh losses.
These are given, illustrative constant efficiencies at steady operation with no changing stored
energy. They are not a motor performance prediction. The accounted losses leave the useful-flow path rather than
disappearing; this example does not predict their temperature or physical mechanism.
Efficiency figures are only comparable when the boundary is the same. A
motor efficiency, a drive efficiency, and a system efficiency measured
from the wall socket to the load are three different numbers for the same machine, and the largest
of them is the one a datasheet prefers to print. Say which one you mean.
Sources
Sources
Supporting detail: Addendum 38 — Where these values were checked.
Engineering Fundamentals/Power Transmission
Belt, Chain and Gear Drives
Choose a drive by shaft spacing, timing, speed and environment, then check its load rating and maintenance needs.
Three ways to carry rotation from one shaft to another
Three ways to carry rotation from one shaft to another
A drive transfers motion and turning effort from a driver to a driven shaft. Belts and chains bridge a gap. Gears engage directly and fit into a compact housing. Start with the job the drive must do, then choose the parts.
Three transmission paths, drawn schematically. A belt or chain lets the shafts sit farther apart without adding an intermediate shaft.
Gears, chains and timing belts are positive drives: engagement maintains a tooth-count ratio without ordinary frictional slip. Flat and V-belts are friction drives: their grip depends on friction and tension, so slip can change the speed ratio.
Positive engagement does not mean perfect positioning. Tooth clearance, elastic deflection and chain speed ripple still matter. For ratios, compound trains and losses, use Gear Ratios. For turning effort and power, use Torque and Power and Efficiency.
Choose a shaft arrangement, a timing requirement, a speed range and an environment. Change one requirement at a time and watch which reason changes. “Close” allows a compact gear mesh; “separated” needs a flexible span. These are qualitative screening rules, not a component sizing tool.
Try this on paper: two separated parallel shafts must stay synchronized in a clean, lubricant-sensitive area. A timing belt is a useful starting candidate: its teeth maintain timing and the belt mesh needs no oil. Flat and V-belts cannot guarantee timing. An ordinary chain needs lubrication; a single gear pair cannot bridge the chosen gap without making the gears much larger.
Now remove the timing requirement: flat or V-belts become candidates. Bring the shafts close together inside a lubricated housing: gears become candidates. Each change removes a different constraint.
Compare timing, space and upkeep side by side
Compare timing, space and upkeep side by side
Typical tendencies for correctly selected industrial drives; actual ratings come from the chosen product.
Question
Flat / V-belt
Timing belt
Roller chain
Gear pair
Center distance
Useful across separated shafts
Useful across separated shafts; check available lengths
Useful across separated shafts; manage slack
Close shafts; size and mesh set spacing
Slip and timing
Can slip; unsuitable for fixed timing
Positive; matched teeth engage
Positive average ratio; clearance and speed ripple remain
Positive ratio; backlash matters on reversal
Noise
Usually quiet; absorbs vibration
Often quiet, but tooth engagement can make noise
Link engagement becomes noisier at speed
Spur teeth can whine; helical engagement is smoother
Lubrication
Belt contact runs dry
Belt contact runs dry
Ordinary chain needs lubricant at its joints
Most loaded metal gears need lubrication
Cost
Often low initial cost
Matched toothed parts usually cost more than basic friction belts
Include sprockets, lubrication and replacement
Precision gears, bearings and housing can raise initial cost
Check oil/grease, seals, tooth condition and alignment
Belt contact running dry does not mean the shaft bearings need no lubrication. A sealed gearbox can keep lubricant away from a product; an exposed chain generally cannot. Special materials and lubrication-free products need their own ratings.
Turn a shortlist into a rated drive; Checklist; Practice
Turn a shortlist into a rated drive
Record shaft directions, center distance, available space and adjustment travel.
Specify input speed, required output speed, power and torque, including starts and shock loads.
Decide whether the job needs synchronized motion, low noise or accurate reversal.
Check temperature, abrasive dust, water and chemicals against the material and lubricant ratings.
Use the manufacturer's selection procedure to check size, service factor, wrap or tooth engagement, shaft loads and bearings.
Plan inspection access, replacement parts, lubrication and the total cost over the drive's life.
A bigger pitch is not a complete strength rating. Width, material, speed, tooth count and duty also matter. A drive that fits the space can still fail the load check.
Supporting detail: Addendum 39 — What the explorer assumes, and where to check a selection.
Engineering Fundamentals/Power Transmission
Keys and Keyways in Shaft-Hub Connections
Trace torque through a keyed shaft-hub joint, identify common key forms, and distinguish key fit from axial retention.
A key joins the shaft slot to the hub slot to transmit torque
A key joins the shaft slot to the hub slot to transmit torque
A key is a separate piece fitted between a shaft and the bore of a hub, the part of a pulley, sprocket or gear that fits around the shaft. Contact between the key and slot faces transfers turning force. Here, keyseat means the recess in the shaft and keyway means the matching slot in the hub. Other references sometimes use keyway for both; always identify which part is being cut.
Schematic parallel-key joint. Clearances are exaggerated; obtain dimensions and fits from the drawing.
Trace the turning load through the connection: shaft slot face → key → hub slot face, or the reverse when the hub drives the shaft. At the rim, the pulley, sprocket or gear transfers the load through its belt, chain or mating gear teeth. Not every hub is keyed; check how the actual assembly connects the hub to the shaft.
Identify the key by its cross-section and seating shape; Practice
Identify the key by its cross-section and seating shape
Key
Recognizing feature
Square parallel key
Equal width and height in cross-section; uniform section along its working length.
Rectangular parallel key
Unequal width and height; uniform section along its working length.
Woodruff key
A segment of a disk, with a curved bottom seated in a matching circular recess in the shaft.
Gib-head key
A tapered key with a projecting head that provides a place to engage it for removal.
Supporting detail: Addendum 40 — Public reference for key forms.
Check key fit and axial retention as separate requirements
Check key fit and axial retention as separate requirements
For a parallel key, the side fit controls how the turning load is carried. Excessive side clearance permits movement; an overly tight fit can prevent assembly. Verify the specified top clearance too. A tapered key has a different seating action, so do not apply a parallel-key fit rule to it.
Use the drawing's key designation, dimensions and tolerances. Do not choose a key size from shaft diameter alone or assume that half the key height belongs in each part.
The key does not by itself define how the hub is held against movement along the shaft. Check the assembly drawing for axial retention as well as torque transmission. A hub that turns with the shaft is not necessarily secured against sliding along it.
Bearings support the shaft relative to the housing; the keyed hub transfers torque between the shaft and the attached rotating part. For the bearing arrangement and the shaft's axial location, see Shaft Support and Axial Adjustment.
Distinguish friction belts from timing belts, read belt and pulley terminology, and recognize common wear patterns.
Flat and V-belts grip; timing belts engage teeth
Flat and V-belts grip; timing belts engage teeth
Flat belt
A broad, flat band transmits force through friction against a pulley. Useful for smooth, quiet motion and long spans when the drive is designed for them. Tracking and tension matter.
V-belt
A trapezoidal section runs in a matching V-groove. Contact at the sides gives a wedging action that increases grip. The belt should not rely on rubbing the bottom of the groove.
Timing / synchronous belt
Teeth on the belt engage matching grooves in the pulleys. Load is carried by this engagement, so the drive keeps its tooth-count ratio without frictional slip in normal operation.
Contact shape determines how force crosses from pulley to belt. Sketches show the principle, not a manufacturing profile.
Timing does not come from extra tension. It comes from matching teeth. An undertensioned or overloaded timing belt can jump teeth or strip them; that is a fault, not its normal way of transmitting power. A notched V-belt remains a friction belt: relief notches for bending do not make it a timing belt.
Belt contact transfers load at the pulley rim; the pulley still needs a connection to its shaft. For a keyed pulley, follow the torque path through the key and hub. Other pulley mountings use different connections.
Read length, tension and wrap before ordering
Read length, tension and wrap before ordering
Pulley / sheave
The wheel that carries a belt. “Sheave” is commonly used for a grooved belt pulley. A timing pulley has matching tooth grooves.
Pitch and pitch length
Timing-belt pitch is the spacing between adjacent tooth centers along the pitch line. Pitch length is the loop length along that reference line, near the tensile cords. It is not the outside circumference. Match pitch and tooth profile to the pulley.
Tension
The pulling force along the belt. The difference between the loaded and return spans transmits torque. Installation tension keeps the belt seated; too little encourages slip or tooth jumping, and too much loads belts and bearings.
Wrap angle
The angle through which the belt contacts a pulley. Less wrap gives a friction belt less contact and a timing belt fewer teeth in engagement. Check the smaller pulley in particular.
Catalogs may specify inside, outside, datum, effective or pitch lengths. Use the length convention and measuring method for that belt family; do not substitute a tape measurement of the outside for the catalog value.
One-stage reminder: nout = nin × Ddriver / Ddriven using matching effective/pitch diameters and assuming no slip. For timing belts, use tooth counts N in place of diameters. Write the reduction as i:1, where i = input speed / output speed. Follow Gear Ratios for the ratio method and Rotation and Linear Speed for belt linear speed.
Here N means teeth and n means rotational speed. Some class slides use n for teeth and ω for angular speed; check the quantity, not just the letter.
Choose a belt for the load and environment
Choose a belt for the load and environment
Belts can span separated shafts, soften vibration and avoid oil at the transmission contact. Flat and V-belts suit jobs where a small speed variation is acceptable. Choose a timing belt when the shafts must stay synchronized. Compare the alternatives in Belt, Chain and Gear Drives.
Check belt section or tooth profile, width, minimum pulley size, available length, wrap, power rating, temperature and chemical compatibility. There is no single maximum speed or temperature range for every belt. Reinforcement cords limit stretch, but the belt still needs correct alignment and installation tension.
Some specially designed flat-belt layouts connect nonparallel shafts. That does not make misalignment acceptable in an ordinary V-belt or timing-belt installation. Frictional slip may soften an overload, but it can also generate heat and destroy the belt; it is not a guaranteed overload-protection device.
Use the wear pattern to find the cause; Practice
Use the wear pattern to find the cause
Fault clues to investigate with the drive safely isolated.
Symptom
Possible cause to check
Squeal, glazing or excess heat on a friction belt
Low tension, overload, contamination or worn pulley grooves can reduce grip.
Frayed edges or the belt tracking to one side
Pulley alignment, damaged flanges and shaft movement.
Cracks or hardening
Age, heat, chemical attack or repeated bending around an unsuitable pulley.
Missing timing-belt teeth or lost timing
Overload, inadequate tension, poor engagement, debris or worn pulleys.
Inspect the pulleys as well as the belt. Replacing the worn part without fixing its cause often repeats the failure. Follow the product's tension and inspection instructions; use Equipment Operating Procedure before touching the drive.
Supporting detail: Addendum 41 — Manufacturer references for belt geometry and faults.
Explore how pulley size and spacing change belt length and wrap; Interactive; Practice
Explore how pulley size and spacing change belt length and wrap
Use pitch diameters D (large) and d (small), and center distance C in one length unit. For an open belt, the approximate pitch length is L ≈ 2C + π(D + d)/2 + (D − d)²/(4C). The last term is the correction for unequal pulleys. Increasing C increases length and brings small-pulley wrap closer to 180°; the no-slip speed ratio stays D/d.
Real belts come in standard lengths from the manufacturer's catalog. Pick the nearest stock length in the correct length convention, then use “Enter L → find C” to estimate the required shaft spacing. These calculations do not set installation tension or replace the manufacturer's selection procedure.
Open belt: D = 200, d = 100 mm; n_small = 1200 r/min
Belt pitch length L (approx., mm)
1277.49
Center distance C (mm)
400
Speed ratio n_small / n_large
2
Large-pulley speed (r/min)
600
Belt speed (m/min)
376.991
Small-pulley wrap (degrees)
165.638
Unequal-pulley correction (mm)
6.25
Less wrap means less grip for a friction belt and fewer teeth engaged for a timing belt. This geometry model does not rate load capacity.
Worked example: D = 200 mm, d = 100 mm, C = 400 mm and n_small = 1200 r/min. L ≈ 800 + 150π + 6.25 = 1277.49 mm. The inverse returns C ≈ 400 mm. Ratio = 2; n_large = 600 r/min; v = π × 100 × 1200 / 1000 ≈ 376.99 m/min; wrap ≈ 165.64°.
Supporting detail: Addendum 42 — Derive the inverse and check speed and wrap.
Recognize chain components, decode ANSI pitch numbers, and distinguish ISO chain series before choosing sprockets.
Sprocket teeth engage a chain of moving joints
Sprocket teeth engage a chain of moving joints
A chain drive is a positive drive: sprocket teeth engage the chain instead of relying on frictional grip. It can bridge separated shafts and carry substantial load, but its joints and sprockets need attention.
Pitch, p
The center-to-center distance between adjacent chain pins. A chain's pitch must match its sprocket.
Roller
A sleeve that turns around a bush as it contacts a sprocket tooth. Some small chains are bush chains and have no separate roller.
Link
A connecting unit of the chain. Ordinary roller chain alternates inner links, carrying bushes and rollers, with outer links, carrying pins and side plates.
Sprocket
The toothed wheel that engages the chain. Tooth count sets the speed relationship; tooth shape and width must suit the chain series.
Master / connecting link
The link used to join the ends into a loop. Use the specified type and installation method; retention and strength depend on the product.
Pitch measures joint spacing, not roller diameter or the length of two links together. Side view is simplified; the pin sits inside the bush and roller.
The chain engages the sprocket teeth, but torque must also pass between each driven or driving sprocket and its shaft. A keyed sprocket uses a key between the shaft and hub; tooth engagement alone does not explain that connection.
Read #25, #35 and #40 as pitch codes
Read #25, #35 and #40 as pitch codes
For the common ANSI short-pitch chain numbers here, remove the final digit of the base number and divide the remaining number by 8 to get pitch in inches. Thus #40 uses 4/8 in, not 40/8 in. #100 uses 10/8 in.
Common ANSI designation examples, checked against Tsubaki's chain guide and sprocket catalog.
Base number
Pitch calculation
Pitch
Construction clue
#25
2/8 in
0.250 in = 6.35 mm
Final 5: bush chain, no separate rollers
#35
3/8 in
0.375 in = 9.525 mm
Final 5: bush chain, no separate rollers
#40
4/8 in
0.500 in = 12.70 mm
Final 0: roller chain
#41
4/8 in
0.500 in = 12.70 mm
Narrow variation; not identical to #40
#100
10/8 in
1.250 in = 31.75 mm
Two digits remain before dividing by 8
A suffix such as -1 or -2 counts parallel strands: simplex or duplex. #40-2 still has a 0.500 in pitch. Heavy-series suffixes and manufacturer prefixes carry other information; do not apply the pitch shortcut to every chain product code.
Supporting detail: Addendum 43 — Checked public wording behind the ANSI numbers.
“Metric chain” still needs a series and a pitch
“Metric chain” still needs a series and a pitch
ISO chain data are commonly tabulated in millimeters. That does not make every pitch a whole number of millimeters. ISO 606 covers both A-series chains derived from American practice and B-series chains derived from European practice.
Selected B-series simplex chains from Renold's public tables.
Designation
Pitch
05B-1
8.000 mm
06B-1
9.525 mm
08B-1
12.700 mm
10B-1
15.875 mm
The common 06B, 08B and 10B sizes correspond to 6/16, 8/16 and 10/16 in pitch. Use the table for the exact designation: small sizes such as 05B do not follow that shortcut. B identifies the series; -1 identifies one strand.
Same pitch does not mean interchangeable. #40 and 08B both have 12.7 mm pitch, but roller diameter and inner width differ. Check series, pitch, width, roller diameter and strand count when matching a sprocket or replacement link.
Supporting detail: Addendum 44 — ISO scope and the source of the millimeter dimensions.
Positive engagement still permits wear and speed ripple; Practice
Positive engagement still permits wear and speed ripple
Chain is worth considering when separated shafts need a fixed average ratio and lubricant and noise are acceptable. Select it for the actual power, speed, starts, shock loads and environment. Tensile breaking strength is not an allowable continuous working load.
One-stage reminder: nout = nin × Ndriver / Ndriven; reduction i = Ndriven / Ndriver, written i:1. N counts teeth and n is rotational speed. For the reasoning and further stages, use Gear Ratios.
The chain wraps a sprocket as a series of straight links, forming a polygon rather than a perfectly smooth circle. This chordal action produces speed ripple, especially with small sprockets. Backlash and elastic stretch also limit precise positioning, even without ordinary slip.
Wear elongation: pin/bush wear increases joint clearance and measured chain length. The worn chain rides poorly on sprocket teeth and can jump. Take-up removes slack; it does not restore worn joints.
Stiff or seized joints: check lubrication reaching the joints, contamination and corrosion.
Fractured plates or pins: investigate fatigue, overload, misalignment and connecting-link installation.
Hooked or uneven sprocket teeth: inspect the chain and sprockets together and follow replacement limits for that drive.
Use the specified lubricant, alignment and slack. A chain is not installed taut like a belt. Set inspection intervals and wear limits from the maker's guide; isolate the drive before measuring or servicing it. See Equipment Operating Procedure.
Supporting detail: Addendum 45 — Chain selection and maintenance reference.
Few sprocket teeth make the chain surge and bob; Interactive
Few sprocket teeth make the chain surge and bob
A chain can bend only at its pins, so it wraps a sprocket as a polygon with one side per tooth. Even at a perfectly steady sprocket speed, the chain leaving that polygon speeds up and slows down once per tooth, and the span rises and falls with it. Predict how much, then turn the sprocket and watch.
Pin at the top: the leaving span sits at the full pitch radius R and moves at ωR, its fastest.Spanheight×21RR cos(20°)drop1.12 mm9 teeth · #40 chain, p = 12.7 mmleaving →← arrivingR = 18.57 mm · ω constant · to fitTwo pins straddle the top: the span leaves from a flat of the polygon at R cos(180°/N) and moves at ωR cos(180°/N), its slowest.
Pitch radiusR = p / (2 sin(180°/N))
Speed rangeωR cos(180°/N) ≤ v ≤ ωR
Ripple(vmax − vmin) / vmax = 1 − cos(180°/N)
Span riseR (1 − cos(180°/N))
Worked example: #40 chain (p = 12.7 mm) on a 9-tooth sprocket at 120 r/min. R = 12.7 / (2 sin 20°) = 18.57 mm. ω = 120 × 2π / 60 = 12.57 rad/s, so vmax = ωR = 0.233 m/s and vmin = ωR cos 20° = 0.219 m/s. Ripple = 1 − cos 20° = 6.03 %; the span rises and falls 1.12 mm, once per tooth: 18 times a second. With 21 teeth the same chain and speed give 1.12 % and 0.476 mm.
858590909595100100chain speed, % of ωR= span height, % of Rsprocket rotation → one grid division = one tooth9 teeth: 6.03 %21 teeth: 1.12 %Three teeth of rotation. Each pulse is one tooth: the speed peaks when a pin passes the top and dips at the hand-over between pins. More teeth make a shallower, more frequent pulse.
Chordal speed variation by tooth count. Rise is for p = 12.7 mm (#40); ripple percentages do not depend on pitch or speed.
Teeth N
R / p
Ripple (vmax − vmin) / vmax
Same spread ÷ average speed
Span rise (mm)
6
1
13.40 %
14.03 %
1.7
8
1.307
7.61 %
7.81 %
1.26
9
1.462
6.03 %
6.15 %
1.12
10
1.618
4.89 %
4.98 %
1.01
12
1.932
3.41 %
3.45 %
0.836
15
2.405
2.19 %
2.20 %
0.667
17
2.721
1.70 %
1.71 %
0.588
19
3.038
1.36 %
1.37 %
0.526
21
3.355
1.12 %
1.12 %
0.476
25
3.989
0.79 %
0.79 %
0.4
30
4.783
0.55 %
0.55 %
0.333
Read the trace: the speed peaks each time a pin passes the top of the sprocket and dips at the hand-over between pins. Chain speed as a fraction of ωR and span height as a fraction of R follow the same curve, cos θ, where θ is the leaving pin's angle from the top. The ripple percentage depends only on the tooth count. Speed and pitch change the size of the numbers, not the percentage.
Supporting detail: Addendum 46 — Where the formulas come from, and what this model leaves out.
Engineering Fundamentals/Power Transmission
Gear Drives and Tooth Geometry
Compare spur and helical gears, identify tooth dimensions, and match pitch and pressure angle before choosing a gear pair.
Gears transmit rotation by direct tooth contact. They make a compact positive drive, but accurate mounting, tooth compatibility and lubrication matter. This page compares external spur and helical gears on parallel shafts.
Spur gear
Teeth run parallel to the shaft. It is comparatively simple to make and produces no axial thrust from the ideal tooth mesh. Engagement can be noisy at higher speed.
Helical gear
Teeth run at a helix angle around the gear. Contact enters progressively across the face and overlapping teeth share load. This generally gives smoother, quieter operation, with added manufacturing cost.
The inclined helical tooth force also pushes along the shaft. That axial thrust needs a suitable bearing arrangement. A spur gear still loads its bearings radially; “no axial thrust” does not mean “no bearing force.”
The driver supplies power. The pinion is the smaller gear in a pair; it can be the driver or the driven member. An idler passes motion between gears and still needs a shaft or other bearing support. Follow Gear Ratios for direction, tooth-count ratios and compound trains.
Tooth contact and shaft attachment are separate connections. Where a gear hub is keyed to its shaft, the key transfers torque at the hub. Check axial retention separately, especially when the tooth mesh produces thrust.
Measure teeth from the pitch circle
Measure teeth from the pitch circle
The pitch circle is a reference, not the outside edge of the gear. The enlarged sector flattens the arcs for clarity; it is not a cutting profile.
Pitch diameter, d
The diameter of the reference pitch circle. In a standard unshifted pair at its standard center distance, the pitch circles roll together without slipping.
Module, m
Metric tooth size: m = d/N, with d in millimeters and N teeth. Larger module means larger teeth.
Diametral pitch, Pd
Inch-based tooth size: Pd = N/d, with d in inches. More teeth per inch of pitch diameter means smaller teeth. Do not confuse it with circular pitch, the distance along the pitch circle between successive teeth.
Pressure angle, α
The angle between the line of action (the contact-force direction, neglecting friction) and the common tangent to the pitch circles at the pitch point. It describes tooth geometry, not the helix angle.
Addendum / dedendum
Radial tooth height from pitch circle to tip / radial depth from pitch circle to root. Neither is a diameter difference by itself.
Backlash
Clearance between mating tooth flanks. It allows clearance in the mesh but creates lost motion when the load reverses.
Supporting detail: Addendum 47 — Check the size definitions with one gear.
Matching pitch is necessary, but not sufficient
Matching pitch is necessary, but not sufficient
Ordinary spur gears intended to mesh must share module or diametral pitch and pressure angle. Matching outside diameter or tooth count does not establish compatibility. Check the tooth system, center distance, clearance and manufacturer's mating information too.
For external helical gears on parallel shafts, match tooth size, pressure angle and helix angle. Use one right-hand and one left-hand gear (teeth slanting in opposite directions), and confirm the manufacturer's mating specification. Equal tooth counts are not required.
Supporting detail: Addendum 48 — Normal and transverse measurements use different planes.
A larger tooth size can support more load when other conditions are comparable, but pitch alone cannot determine capacity, backlash or achievable reduction. Material, face width, heat treatment, alignment and speed remain part of the design.
Supporting detail: Addendum 49 — Primary references for the geometry and helical mesh.
Gear damage tells you where the load went
Gear damage tells you where the load went
Choose gears for compact packaging, a positive ratio and a supported shaft arrangement. Choose helical teeth when smoothness and noise justify their cost and thrust bearings. Check tooth bending strength, surface durability, speed, lubricant, seals and bearing loads before approving a pair.
Common gear faults and conditions to investigate.
Damage
What to check
Scoring or scuffing: streaked, torn tooth surfaces
Lubricant supply and type, excess temperature, contamination and load.
Broken tooth or root crack
Overload, repeated bending fatigue, impact and material condition.
Pitting / spalling: small pits or flakes leaving the surface
Repeated contact stress, lubrication and local load concentration.
Wear concentrated at one edge
Shaft/bearing alignment, deflection and tooth contact pattern.
A symptom is a clue, not a unique diagnosis. Correct the cause before replacing parts. Most loaded metal gear sets need a controlled lubricant supply; some specially selected materials can run dry. Follow the product data and Equipment Operating Procedure for access.
Choose a thread form for the load, read an inch or metric callout, and identify which way a screw advances.
A fastener holds parts together; a power screw moves a load
A fastener holds parts together; a power screw moves a load
A thread is a ridge wrapped around a cylinder. A matching internal thread in a nut follows that ridge. Relative rotation can produce straight-line travel along the screw's axis.
A machine screw usually holds parts together. A lead screw uses the thread to position or drive a load: a slide, a vise jaw, or a linear actuator. Belts, chains and gears commonly transfer rotation between shafts; a lead screw converts rotation into linear motion. See Lead Screws for the calculations.
Keep four descriptions separate: form is the thread's cross-sectional shape; series selects diameter and pitch combinations; hand determines direction; starts count the separate helices. A helix is the spiral path around the cylinder.
Match the thread form to fastening, repeated travel, or one-way thrust
Match the thread form to fastening, repeated travel, or one-way thrust
Profiles cut through the screw axis. These drawings compare shapes, not manufacturing dimensions. The load-bearing side of a thread is its flank.
Thread-form trade-offs for sliding screw-and-nut contact.
Form and use
What it offers
What it costs
Square: power screws and jacks
High efficiency relative to angled flanks under otherwise comparable conditions.
Difficult, expensive machining; wear adjustment is difficult.
V / machine-screw thread: bolts and fastening screws
Widely available fasteners; mass production by rolling makes standard parts economical.
Flank wedging increases friction, so it is a poor choice for efficient repeated power transmission.
ACME / metric trapezoidal: vises, clamps and linear actuators
Easier machining than square; a broader thread root provides a sturdier profile than a comparable square thread. Split-nut (an adjustable, divided nut) arrangements can take up clearance.
Flank wedging increases friction relative to square. A precision drive screw can cost more than an ordinary stock fastener.
Buttress: heavy axial thrust (push along the screw) predominantly in one axial direction, such as a screw press
A nearly perpendicular working flank limits wedging in the intended load direction; the sloping back supports the thread.
Its strength and efficiency advantages are directional. A special asymmetric profile and matching nut affect manufacturing and cost.
No thread form wins every comparison. Actual strength also depends on diameter, pitch, engaged length, material and the failure being checked. ACME is not automatically stronger than every V thread. Nor does its name guarantee a larger lead. ACME and metric trapezoidal are related forms, not interchangeable parts.
Supporting detail: Addendum 50 — Why the efficiency and strength comparisons need conditions.
No radial wedging (outward force on the nut) does not mean no wear
No radial wedging (outward force on the nut) does not mean no wear
In the ideal square-thread geometry, axial load does not create the outward wedging associated with angled flanks. That reduces a source of radial loading on the nut. The loaded surfaces still slide against each other. Friction, lubrication, materials, load and speed still affect wear.
Wear can increase backlash: clearance that must be taken up after reversing direction before the load moves. An adjustable nut can reduce that clearance; adjustment does not restore lost material or guarantee longer life. Do not infer nut life from the thread profile alone.
Supporting detail: Addendum 51 — Where wear and operating limits enter the selection.
Inch callouts count threads; metric callouts state pitch; Practice
Inch callouts count threads; metric callouts state pitch
Pitch is the axial distance between adjacent thread crests. Inch fastener callouts commonly give threads per inch (TPI), so pitch = 1 / TPI in inches. Metric callouts give pitch directly in millimetres.
Selected callouts transcribed from checked public standard sources; pitches in the last column are calculated.
Callout
Read it as
Pitch
1/4-20 UNC
Nominal diameter 1/4 in; 20 threads per inch; Unified coarse series
1/20 = 0.050 in
1/4-28 UNF
Nominal diameter 1/4 in; 28 threads per inch; Unified fine series
1/28 ≈ 0.03571 in
M6 × 1.0
Metric thread; nominal diameter 6 mm; pitch 1.0 mm
1.0 mm
Fine means a smaller pitch at the same nominal diameter. It does not mean a better-quality thread. Metric threads also have coarse and fine pitch choices. The 6 in M6 is a diameter, not a pitch; the 20 in 1/4-20 is a count per inch, not a lead.
These are basic size-and-pitch callouts, not complete manufacturing specifications. Fit and tolerance information may follow them. A fastener-series label does not tell you the efficiency of a lead screw; for a multiple-start drive, obtain both pitch and starts, or the lead directly.
Supporting detail: Addendum 52 — The exact standard entries used here.
Right-hand and left-hand threads advance in opposite directions
Right-hand and left-hand threads advance in opposite directions
Fix the nut and look along the screw from the end you turn. Clockwise turns a right-hand screw away from you into the nut. The same clockwise rotation moves a left-hand screw toward you. Reverse the rotation and the travel reverses.
Same observer, same rotating member, same clockwise rotation. State all three before assigning a travel direction.
If the screw is held against axial motion and the nut travels instead, the nut moves opposite to the screw travel just described. Handedness changes the direction, not the magnitude of travel per revolution.
Supporting detail: Addendum 53 — Direction reference.
Pitch times starts gives lead. Use lead to convert rpm into travel speed and torque into force, with efficiency applied only to the force conversion.
Pitch is thread spacing; lead is travel per revolution
Pitch is thread spacing; lead is travel per revolution
Lead = pitch × number of starts. This is the distinction to get right before calculating either speed or force.
A start is one continuous helical ridge. A single-start screw has one ridge, so its lead equals its pitch. A triple-start screw has three interleaved ridges: follow one ridge through a full turn and it advances three pitch distances.
Imagine unwrapping the cylindrical surface. Top and bottom are the same angular position one full turn apart. Pitch is measured along the axis between adjacent ridges; lead follows the same ridge through a turn.
At the same pitch, adding starts increases travel per turn. At the same torque it reduces theoretical force. The thread's cross-sectional form and its number of starts are separate choices; see Screw Threads.
Supporting detail: Addendum 54 — Check the definition, not just the label on a catalog.
Multiply rpm by lead to find linear speed
Multiply rpm by lead to find linear speed
For an engaged screw and nut, with the nut restrained from rotating, v = nL. Here n is screw speed in revolutions per minute and L is lead in distance per revolution. The result is distance per minute. Divide by 60 for distance per second.
A triple-start screw with 1.5 mm pitch has L = 1.5 × 3 = 4.5 mm/rev. At 480 rpm, v = 480 × 4.5 = 2,160 mm/min = 36 mm/s.
Do not multiply that speed by efficiency. The teaching rule is: “RPM → velocity is 100% efficient unless the screw is malfunctioning; all efficiency losses are found in the torque → force conversion.” This describes a positive-drive motion relationship, not 100% energy efficiency. It is the same tooth-count principle used in Gear Ratios.
Use the actual screw rpm. If the motor slows under load, the lower rpm gives a lower travel speed. Backlash at reversal and elastic deflection can affect positioning without being an efficiency factor on speed. These calculations describe steady engaged travel, after clearance is taken up. See Rotation and Linear Speed for the general rotation-to-travel connection.
Divide torque times 2π by lead, then apply efficiency
Divide torque times 2π by lead, then apply efficiency
For steady motion driving a resisting axial load, Ftheoretical = 2πT / L and Factual = η × Ftheoretical. Here T is input torque and η (eta) is efficiency written as a decimal: 40% is 0.40.
Make the length in torque match the length in lead.
Torque
Lead for force calculation
Force
N·m
metres per revolution (mm ÷ 1,000)
N
lbf·in (often written lb-in)
inches per revolution
lbf
To find the torque required for a target actual force, rearrange: T = FL / (2πη). For the same load and lead, lower efficiency requires more torque. Keep the efficiency boundary consistent: a whole screw assembly efficiency includes losses in the bearings or collar (a supporting thrust-contact surface) as well as the threads.
Supporting detail: Addendum 55 — Derive the 2π from equal power, or one revolution of work.
Experiment: more starts change speed and force in opposite ways; Interactive
Experiment: more starts change speed and force in opposite ways
Predict first: keep pitch, rpm, torque and efficiency fixed, then change from one start to three. Lead and speed triple; theoretical force falls to one third. The same force ratio holds when efficiency is held fixed.
Static comparison / print example: pitch 2 mm, 300 rpm, torque 1.2 N·m, given efficiency 40%.
Same pitch and input, different starts.
Starts
Lead
Speed
Ideal force
Actual force
1
2 mm/rev
10 mm/s
3,770 N
1,508 N
3
6 mm/rev
30 mm/s
1,257 N
503 N
Changing efficiency to 20% halves each actual force; both speeds stay the same. Real efficiency can change with lead, lubrication and load. Here it is an independent input so the two effects can be studied separately.
Worked actuator: keep inch torque and inch lead together; Practice
Worked actuator: keep inch torque and inch lead together
A single-start ACME actuator has 0.20 in pitch, runs at 900 rpm and receives 12 lbf·in of torque. Its assembly efficiency is given as 60%. Find travel speed and useful axial force.
L = 0.20 × 1 = 0.20 in/rev.
v = 900 × 0.20 = 180 in/min = 3 in/s.
Ftheoretical = 2π × 12 / 0.20 = 376.99 lbf.
Factual = 376.99 × 0.60 ≈ 226 lbf.
The 60% belongs in step 4, not step 2. It is an example input, not an efficiency assigned to every ACME screw.
Worked vise: turn hand force into torque before finding clamp force; Practice
Worked vise: turn hand force into torque before finding clamp force
For an illustrative square-thread vise, a 120 N hand force acts perpendicular to the handle at a radius of 0.18 m from the screw axis. Pitch is 4 mm with one start. Assume a given overall tightening efficiency of 30%; this is not a measured or universal vise efficiency.
Use torque = radius × perpendicular force: T = 0.18 × 120 = 21.6 N·m. Radius is the distance from the axis to the hand, not necessarily the full handle length.
This is a tightening estimate using the supplied efficiency. It is not a vise rating or a prediction of residual force after the hand stops turning. A separate free-travel calculation at 24 rpm gives 24 × 4 / 60 = 1.6 mm/s; the jaws do not continue at that speed through a rigid clamped part.
After a feed screw reverses, the handwheel turns through the thread clearance before the carriage moves. Predict that dead band from clearance and lead, and finish every approach in one direction.
The dial counts screw rotation; the indicator finds the carriage
The dial counts screw rotation; the indicator finds the carriage
A handwheel dial does not measure the carriage. It counts how far the screw has turned and multiplies by the lead. That is the carriage's travel only while the screw keeps pushing the nut in one direction.
A screw and its nut need some clearance between their thread flanks (a flank is the sloping side of a thread). After the screw changes direction, it must turn through that clearance before its other flank meets the nut and the carriage moves again. That clearance is backlash, the same idea defined for threads in Screw Threads and for gear teeth in Gear Drives and Tooth Geometry. The turn spent crossing it is lost motion: input that produces no output.
Dial reading: travel predicted from screw rotation, turns × lead. See Lead Screws.
Carriage position: where the carriage really is, as an indicator touching it would show.
The difference is zero after a forward approach (the direction the dial was zeroed in) and one full clearance after a reverse approach.
Supporting detail: Addendum 56 — Where the definition comes from.
Experiment: reverse the handwheel and watch the carriage wait; Interactive
Experiment: reverse the handwheel and watch the carriage wait
What the lab does: a handwheel turns an axially fixed lead screw. The dial reports travel calculated from screw rotation; an indicator on the carriage reports where the carriage really is. With a total axial clearance B between screw and nut flanks, the two agree only while the screw keeps pushing in the direction the dial was set in.
Dead band after a reversal = clearance ÷ lead, as a fraction of a turn:
angle = 360° × B ÷ Ldial divisions = B ÷ (L ÷ 100) on a dial with 100 divisions per turn.
Worked example: lead L = 5 mm/rev, so one division is 0.05 mm. Clearance B = 0.20 mm. Angle = 360° × 0.20 ÷ 5 = 14.4°; divisions = 0.20 ÷ 0.05 = 4. For four divisions after the reversal the dial changes and the carriage does not.
Handwheel dial reading 0.80 mm: 0 turns and 16 divisions of 0.05 mm.01020304050607080900.80mmIndicator on the carriage reads 1.00 mm.01020304050607080901.00mm
Driven forward to 1.00 mm, then reversed four divisions: the dial reads 0.80 mm (the shaded graduations passed under the index) while the indicator still reads 1.00 mm. Illustrative dial, lead 5 mm, clearance 0.20 mm.Hysteresis loop: carriage position against dial reading. The band between the forward-approach line and the reverse-approach line is 0.20 mm wide along the dial axis. Current dial 1.00 mm, carriage 1.00 mm.−0.30.00.30.50.81.01.3−0.30.00.30.50.81.01.3B = 0.20 mmDial reading from screw rotation (mm)Carriage from indicator (mm)forward approach: carriage = dialreverse approach: carriage = dial + BForward 0 → 1.00 mm, back to 0, forward to 1.00 mm again. Each reversal runs along a flat step 0.20 mm long, so the path is a loop B wide measured along the dial axis.Axial section through the thread, drawn riding on the carriage. Screw flank pushing the nut toward +X. To scale: lead 5 mm, clearance 1.00 mm (illustrative 30-degree thread form).+X →Screw flank pushing the nut toward +Xbronze nut, moves with the carriagesteel screw, turns but never slidesDriving forward · To scale: lead 5 mm, clearance 1.00 mmAxial section through the thread, drawn riding on the carriage. Nut held in the clearance: no flank touching. To scale: lead 5 mm, clearance 1.00 mm (illustrative 30-degree thread form).+X →Nut held in the clearance: no flank touchingbronze nut, moves with the carriagesteel screw, turns but never slidesReversed part way · To scale: lead 5 mm, clearance 1.00 mmAxial section through the thread, drawn riding on the carriage. Screw flank pushing the nut toward −X. To scale: lead 5 mm, clearance 1.00 mm (illustrative 30-degree thread form).+X →Screw flank pushing the nut toward −Xbronze nut, moves with the carriagesteel screw, turns but never slidesDriving back · To scale: lead 5 mm, clearance 1.00 mmThe same three moments in the thread, drawn to scale for lead 5 mm and clearance 1.0 mm (the exaggerated clearance of the 3D model). The heavy blue line marks the flank in contact. Reversing moves the contact from one flank to the other; between the two, nothing pushes the carriage.
Landing on 25.00 mm after overshooting to 25.60 mm (lead 5 mm, clearance 0.20 mm). The dial was zeroed after a forward approach, so it equals the carriage position only for forward approaches:
Same dial number, two approaches.
Method
Dial moves
Dial
Carriage
Error
Reverse straight to the number
25.60 → 25.00 mm
25.00 mm
25.20 mm
+0.20 mm
Back past it, approach forward again
25.60 → 24.50 → 25.00 mm
25.00 mm
25.00 mm
0.00 mm
Reversing straight to the number stops the carriage one full clearance away from the dial reading, still on the overshoot side: the dial shows 25.00 mm while the carriage is at 25.20 mm. Backing past the target by more than the clearance and finishing in the original direction puts the screw back on the flank the dial was set against.
Model limits: rigid parts and a kinematic dead band only. Friction is assumed to hold the carriage still inside the clearance, and nothing else pushes it along the axis; there is no force, stiffness, preload or stick-slip model. Lead, clearance and the 3D dimensions are illustrative and exaggerated, not a standard thread or a measured machine.
Predict the dead band: clearance divided by lead, as a fraction of a turn
Predict the dead band: clearance divided by lead, as a fraction of a turn
Once the screw reverses, the carriage stays still until the screw's helix has moved one full clearance B. One turn moves the helix one lead L, so the dead band is B ÷ L of a turn.
dead-band angle = 360° × B ÷ L
dead-band divisions = B ÷ (value of one division); with 100 divisions per turn, one division is L ÷ 100.
Same clearance, two leads (illustrative values, 100-division dial).
Lead L
One division
Clearance B
Dead band
5 mm/rev
0.05 mm
0.20 mm
4 divisions = 14.4°
2 mm/rev
0.02 mm
0.20 mm
10 divisions = 36°
The carriage error after a reverse approach is the same 0.20 mm in both rows. A finer lead only spreads that same clearance over more of the handwheel turn.
Land on a dimension: finish every approach in the direction the dial was set
Land on a dimension: finish every approach in the direction the dial was set
If you overshoot a target, turning straight back to the number leaves the carriage one clearance away from it, because the screw is now pushing on the other flank. Instead:
Back the handwheel past the target by more than the backlash.
Turn in the original direction again and stop on the number.
The same reasoning applies when setting a dial. MIT's 2.670 milling notes say to “be certain that the backlash in the mechanism driving the table is taken up prior to setting the dial indicator”. A dial set with the clearance taken up in one direction reads true for approaches in that direction. For edge finding, Mill Indicators and Part Zero repeats the touch from the same direction for the same reason.
Supporting detail: Addendum 57 — A readout that measures the slide, and when the clearance still matters.
What the lab model includes and leaves out
What the lab model includes and leaves out
Included: a rigid screw that turns but never slides along its axis, a nut fixed to the carriage, and a total axial clearance B. The carriage position c stays within B/2 of the screw's helical phase s = −Lφ/360° (right-hand thread, φ the screw rotation); inside that band it does not move.
Assumed: friction holds the carriage still inside the clearance, and no outside force pushes it along the axis.
Left out: forces, friction values, stiffness and elastic wind-up, preload, stick-slip and wear. Drives designed to remove the clearance, such as preloaded ball nuts or adjustable split nuts, are beyond this model.
Illustrative: the leads, clearances and the 3D screw (5 mm lead, 1.0 mm clearance, 30° flanks) are chosen to be seen, not taken from a standard thread or a measured machine.
For drive design in depth, Alexander Slocum's Precision Machine Design (1992) covers actuators and transmissions in Chapter 10, including section 10.8, Linear Power Transmission Elements.
Mill around an island: X and Y backlash change the material left behind; Interactive
Mill around an island: X and Y backlash change the material left behind
A perfect 4 mm diameter cutter makes one contour groove around a 24 mm circular island. The dashed outline is the intended island; span errors compare with zero backlash. Material in the middle and outside the groove remains: this is not a pocket-clearing path. Only X/Y drive clearance changes.
Cut as intendedExtra cutMissed cut
Zero backlash · X 0.00 / Y 0.00 mmTop view of a contour groove around a circle island. X clearance 0.00 mm, Y clearance 0.00 mm. Complete pass. Shaded cells are swept by the full cutter; the middle is retained material.+X+Y−10010 mm
X span at Y = 024.000 mm0.000 mm error
Y span at X = 024.000 mm0.000 mm error
X only · X 0.50 / Y 0.00 mmTop view of a contour groove around a circle island. X clearance 0.50 mm, Y clearance 0.00 mm. Complete pass. Shaded cells are swept by the full cutter; the middle is retained material.+X+Y−10010 mm
X span at Y = 023.500 mm−0.500 mm error
Y span at X = 023.989 mm−0.011 mm error
Y only · X 0.00 / Y 0.50 mmTop view of a contour groove around a circle island. X clearance 0.00 mm, Y clearance 0.50 mm. Complete pass. Shaded cells are swept by the full cutter; the middle is retained material.+X+Y−10010 mm
X span at Y = 023.989 mm−0.011 mm error
Y span at X = 023.500 mm−0.500 mm error
Both axes · X 0.50 / Y 0.50 mmTop view of a contour groove around a circle island. X clearance 0.50 mm, Y clearance 0.50 mm. Complete pass. Shaded cells are swept by the full cutter; the middle is retained material.+X+Y−10010 mm
X span at Y = 023.500 mm−0.500 mm error
Y span at X = 023.500 mm−0.500 mm error
All four start at the right side and run counterclockwise. Before the plunge, both axes approach the start in their positive directions and the coordinates are calibrated there. On reversal, the actual cutter can stay still along one axis while moving along the other. Its full circular footprint removes material along that path.
The spans above are sections through X = 0 or Y = 0, not a best-fit circle or the greatest overall width. They come from intersections with the swept cutter, not pixel counting. Changing the start, winding or initial seating can change the local shape; do not infer that every circle becomes the same oval.
Approximation: circular paths use 1° chords (under 0.001 mm sag here). These printed diagrams use 0.20 mm cells; the live area shading uses 0.10 mm cells. The millimetre span readings use the underlying swept chords.
The cutter removes the upper layer at one fixed depth. Grey is material still at its original height; the groove floor is not drawn. A boundary pass leaves both an island and the surrounding stock, so it is not a cleared pocket. The dashed line is the intended island boundary, not the cutter-centre path: that path is one cutter radius outside it.
Supporting detail: Addendum 58 — What the model means, and why it is not a prediction for every CNC.
Engineering Fundamentals/Power Transmission
Bearing Types and Loads
Choose the motion to allow, identify the load, then compare plain and rolling-element bearings.
A bearing allows useful motion and restrains unwanted motion
A bearing allows useful motion and restrains unwanted motion
A loose rigid part can move in six independent ways: translate along three axes and rotate about those three axes. These are its degrees of freedom. A bearing transfers load to a support while allowing the motion the machine needs, with low friction.
For a rotating shaft, the goal is usually one remaining freedom: rotation about its own axis. Two spaced radial supports resist sideways movement and tilting; axial location stops the shaft walking lengthwise. A single short bearing does not automatically provide that whole constraint system.
Let x run along the shaft. Translation T means movement along an axis; rotation R means turning about it. This is an ideal rigid-body model; real supports deflect and have clearance.
Bearings guide motion; motors and drives supply it. Belt, chain and gear drives load their supporting shafts. See Torque for turning effort and Shaft Support and Axial Adjustment for the complete support arrangement.
Radial load crosses the shaft; thrust acts along it
Radial load crosses the shaft; thrust acts along it
Radial load acts perpendicular to the shaft axis. Axial load, or thrust, acts parallel to it. Combined load has both components. A bearing's orientation and internal geometry determine which it can carry.
Load direction is relative to the shaft, not to the room: a vertical shaft can have a horizontal radial load.
First selection filter, not a load rating. Check the exact catalog design.
Type
Radial load
Axial load
Combined load
Plain journal, without thrust faces
Yes
No intended capacity
Needs a thrust bearing
Plain footstep or thrust collar face
Needs a journal guide
Yes, against the loaded face
With a radial guide
Deep-groove ball
Yes
Both directions, within rating
Yes, within rating
Angular-contact ball or tapered roller, single row
Yes
Primarily one direction
Yes; opposing bearing needed for reverse thrust
Cylindrical roller, NU or N design
Yes
No intended locating duty
Use another bearing for thrust
Pure thrust ball or cylindrical thrust roller
No
Yes; direction depends on arrangement
No
Do not turn “roller” into “radial only,” or “thrust” into a rule for every product bearing that name. Tapered rollers carry combined loads; some spherical roller thrust designs also accept radial load under specified conditions.
Plain and rolling bearings trade friction, upkeep and cost
Plain and rolling bearings trade friction, upkeep and cost
A plain bearing supports sliding surfaces, often with a replaceable sleeve called a bushing. A rolling-element bearing places balls or rollers between rings. “Anti-friction” is a traditional name, not a promise of zero friction.
Compare the operating conditions as well as the purchase price.
Question
Plain bearing
Rolling-element bearing
Starting versus running resistance?
Breakaway friction can exceed running friction. A hydrodynamic film is not fully established at rest.
Often low starting resistance and a smaller start/run difference; seals, grease and preload still matter.
Lubrication and maintenance?
Dry grades may need no added lubricant; oil-fed designs require the specified supply and cleanliness.
Usually grease or oil lubricated. A sealed, prelubricated bearing still has a finite service life.
Speed?
Dry bushings have material-specific speed and pressure limits. Fluid-film bearings can serve high-speed machinery.
Many suit moderate to high speeds; type, size, lubrication and heat limit speed.
Load and cost?
Simple bushings often cost little initially. Capacity depends on size, material, speed and heat removal.
Precision rings and elements add cost. Roller designs often carry more load than ball designs of similar overall size.
Rolling contact generally reduces resistance compared with sliding contact. It does not guarantee higher efficiency than every fluid-film bearing, nor does a cheap bushing guarantee lower lifetime cost. Include lubrication equipment, replacement, downtime and power loss. Bearing losses contribute to Power and Efficiency and the stage efficiencies discussed in Gear Ratios.
Plain bearings differ in both lubrication and load direction
Plain bearings differ in both lubrication and load direction
Dry or self-lubricating
A suitable polymer, composite or lubricant-containing material supplies a low-friction sliding surface. Follow that material's instructions; adding grease is not automatically an improvement.
Hydrodynamic
Relative motion draws lubricant into a converging gap, forming a pressure-supported film. Starts and stops require attention because the running film depends on motion.
Hydrostatic
An external pressure supply supports the load on a fluid film, including at rest while the supply operates. The pump, flow control and loss-of-pressure behavior are part of the system.
Those are lubrication descriptions. Shape answers a different question: a journal surrounds a shaft to carry radial load; a footstep supports axial load at a shaft end; a thrust collar presents an annular face to carry axial load. An assembly can combine a journal and a collar to handle both components.
Rings carry the load; the cage spaces the rolling elements; Practice
Rings carry the load; the cage spaces the rolling elements
Schematic with seals omitted. A raceway is the track on a ring that the rolling elements contact; ring and raceway are not quite the same thing.
The inner ring fits around the shaft; the outer ring fits in the housing. The rolling elements transfer load between their raceways. The cage maintains spacing and guides the elements.
In a common arrangement the inner ring turns with the shaft while the outer ring stays still. The balls spin about their own axes and orbit around the shaft. The rings do not have to rotate in opposite directions.
Balls have idealized point contact; rollers have idealized line contact. Under load these become finite contact patches. The longer roller contact generally supports more load in a similar overall size. Contact angle, not just element shape, determines thrust capability. Thrust ball and roller bearings place their contact geometry to support axial force.
Supporting detail: Addendum 59 — Manufacturer reading for bearing selection.
Recognize the bearing family by its contact geometry; Interactive
Recognize the bearing family by its contact geometry
Choose a family and compare its section with its end view. A radial bearing surrounds the shaft; a thrust bearing places its load-carrying faces across the shaft axis. Ball, straight roller, tapered roller and barrel roller shapes lead to different contact paths.
Fᵣ is radial load; Fₐ is axial load. Arrows show directions, not ratings. Sections omit the cage; end views expose the elements.
Plain journal / bushing
A sleeve supports a sliding shaft surface. Radial load crosses the sleeve. This unflanged journal does not locate the shaft axially. Manufacturer guide.
Plain thrust face
A collar slides against an annular thrust face. The loaded face reacts axial force in one direction. A journal guide supplies the separate radial support. Manufacturer guide.
Deep-groove ball
Deep, nearly circular grooves surround one row of balls. Primarily radial duty, with axial capacity in either direction within the catalog limits. Manufacturer guide.
Angular-contact ball
Offset shoulders give an inclined contact line. A single row carries radial load and thrust in the shown direction. Opposed bearings handle reverse thrust; this is not a preload-setting drawing. Manufacturer guide.
Self-aligning ball
Two ball rows share one spherical outer raceway. The inner assembly can tilt about the bearing centre. Axial capacity is relatively small; allowable misalignment depends on the product and surrounding parts. Manufacturer guide.
Thrust ball
Balls run between grooved washers facing each other. The single-direction arrangement shown carries axial load only. It still needs separate radial guidance. Manufacturer guide.
Cylindrical roller · NU
Straight rollers run parallel to the shaft axis. The NU example has guiding ribs on the outer ring and no inner-ring ribs, allowing axial displacement. Other rib arrangements have different axial duties. Manufacturer guide.
Needle roller · radial
Long, slender rollers give a shallow radial section. This radial example includes both rings. Some needle assemblies run directly on a suitably prepared shaft; a separate thrust-needle arrangement is a different geometry. Manufacturer guide.
Tapered roller
Conical rollers sit between conical raceways. Raceways and roller axes have a common cone apex on the shaft axis. A single row takes radial load plus thrust toward its small end, as drawn; an opposed bearing takes reverse thrust. Manufacturer guide.
Spherical roller
Two rows of barrel rollers share a spherical outer raceway. The curved outer track permits limited self-alignment. The bearing carries radial and bidirectional axial loads within its ratings. Manufacturer guide.
Cylindrical roller thrust
Roller axes point radially across flat washer faces. The single-direction arrangement shown carries axial load, not radial guidance. Compare its radial roller orientation with the shaft-parallel rollers in the NU bearing. Manufacturer guide.
Spherical roller thrust
Inclined barrel rollers meet a spherical housing raceway. Primarily thrust in one direction, with some radial capacity while axial load is present. The spherical raceway permits limited self-alignment; consult the exact design. Manufacturer guide.
These are original schematic sections, not interchangeable catalog parts. Cage details and seals are omitted from the sections to expose the contact geometry. A self-aligning raceway allows a limited tilt; it does not excuse arbitrary misalignment or eliminate the need for a correctly designed support arrangement.
Read the type, dimensions and suffixes in Bearing Designations and Sizes. The type tells you which catalog to consult; the complete designation and catalog row tell you what fits.
A pillow block is a housing arrangement, not another rolling-element shape
A pillow block is a housing arrangement, not another rolling-element shape
The outside casting provides mounting points. Identify the bearing or insert inside it separately.
A pillow or plummer block supports a shaft from a base. A flange-mounted housing attaches around the shaft to a facing support. Different housings can contain different bearing families. For example, NSK Self-Lube units combine a sealed ball-bearing insert with a pillow-block or flanged housing.
Double a ball bearing's load and its basic rating life falls to one eighth; Interactive; Practice
Double a ball bearing's load and its basic rating life falls to one eighth
L10 is the life that 90% of a large group of identical bearings are expected to reach or exceed. It is neither a guaranteed life nor an average. Change one input below and watch the life curve.
Example bearing: C = 14.0 kN, given for this exercise. A real bearing's C comes from its manufacturer's catalog; this example does not represent a catalog part.
Basic rating life: L10 = (C/P)p in millions of revolutions, with p = 3 for balls and p = 10/3 for rollers. C is the basic dynamic load rating; P is the equivalent dynamic load, taken as given here (for pure radial loading in this exercise, P = Fr). Use the same force units for C and P.
At constant speed n in r/min, L10h = L10 × 10⁶/(60 × n) hours. The years conversion assumes a duty schedule you can change; it does not predict calendar aging.
Static worked example (also used for printing).
Example ball bearing: C = 14 kN (given), P = 2 kN, n = 1500 r/min
L10h versus P: logarithmic vertical scale. Equal vertical steps represent equal life ratios. C and speed stay fixed.L10h (h), log scale30490138112476.44P (kN)
Marked points: current 2 kN → 3811 h; double load 4 kN → 476.4 h. Double the load → 1/8 the life.
C/P = 14/2 = 7; L10 = 7³ = 343 million revolutions. L10h = 343 × 10⁶/(60 × 1500) = 3811 h, or 1.906 years at 2000 h/year. At P = 4 kN, L10 = 42.875 million revolutions and L10h = 476.4 h.
Adjusted life factors (a1, aISO), contamination, lubrication and combined-load X/Y factors are beyond this page.
Read a supported bearing code, then use the manufacturer's catalog for its outside diameter, width and full specification.
Read the basic designation before the extra letters
Read the basic designation before the extra letters
A bearing number is a compact description, not a universal sizing formula. Start with the maker and the bearing family. A basic designation identifies a series and bore; prefixes and suffixes add details. The same letters can mean different things in different families or manufacturers' catalogs.
For the ordinary metric deep-groove example 6205, read 6 | (0)2 | 05: type 6 is deep-groove ball; 02 is the dimension series, with width-series 0 omitted in the written number; bore code 05 means 25 mm. The diameter-series digit 2 is not an outside diameter in millimetres.
Width-series digits can be omitted differently: NSK lists 6005 as 6 | (1)0 | 05, and 6305 as 6 | (0)3 | 05. Parentheses here explain the omitted digit; they are not characters to add to an order. See NSK's bearing-series table.
Recognize the geometry first in Bearing Types and Loads. A matching bore alone does not make two bearings interchangeable.
The same bore can come with a different outside diameter and width; Interactive
The same bore can come with a different outside diameter and width
Compare the three catalog rows below. d is the bore, D the outside diameter and B the width. Their 25 mm bores are equal, while their housing and axial-space requirements differ. The picture keeps one scale so that this difference is visible.
All three are single-row deep-groove ball bearings. The bore code is 05 → 25 mm; the other dimensions below are catalog values, not digit arithmetic.
Same 25 mm bore; different NSK catalog envelopes (mm)
6005: bore 25, outside diameter 47, width 12 mm. Boundary envelope, internal parts omitted.6005 · NSK boundary dimensionsd 25D 47B 12mm · constant drawing scale across the three sizesNSK 6005: 25 × 47 × 12 mm. The drawing shows only the mounting envelope; it is not an internal construction drawing.6205: bore 25, outside diameter 52, width 15 mm. Boundary envelope, internal parts omitted.6205 · NSK boundary dimensionsd 25D 52B 15mm · constant drawing scale across the three sizesNSK 6205: 25 × 52 × 15 mm. The drawing shows only the mounting envelope; it is not an internal construction drawing.6305: bore 25, outside diameter 62, width 17 mm. Boundary envelope, internal parts omitted.6305 · NSK boundary dimensionsd 25D 62B 17mm · constant drawing scale across the three sizesNSK 6305: 25 × 62 × 17 mm. The drawing shows only the mounting envelope; it is not an internal construction drawing.
These are nominal boundary dimensions. Shaft and housing fits, shoulder dimensions, corner radii, internal clearance and tolerances still require the complete catalog entry and the application design.
00, 01, 02 and 03 are the bore-code exceptions
00, 01, 02 and 03 are the bore-code exceptions
Ordinary coded metric bores in the system illustrated here
Bore code
Bore d
How it is read
00
10 mm
Special code
01
12 mm
Special code
02
15 mm
Special code
03
17 mm
Special code
04–96
20–480 mm
Code × 5 mm, where this coding system applies
Thus 6202 has a 15 mm bore, not 10 mm; 6205 has a 25 mm bore. This rule supplies only the bore. It does not calculate D or B.
Do not apply it blindly to miniature, inch, letter-coded or special bearings. Slash forms can state the bore directly: NSK gives 63/22 as 22 mm and 230/560 as 560 mm. Its miniature 688 example has an 8 mm bore. NSK excludes double-direction thrust ball bearings from its general 04–96 rule.
Supporting detail: Addendum 60 — Primary references for the bore-code scope.
Series identify a family; the catalog supplies the envelope
Series identify a family; the catalog supplies the envelope
Examples of NSK metric series, not a universal first-digit decoder
A dimension series selects a standardized size family; it is a table key, not a digit-to-millimetres formula. Series examples follow NSK's designation guide. Different types also use different dimension letters. A tapered bearing distinguishes inner-ring width B, outer-ring width C and assembled width T. Thrust catalogs may label axial height T or H: use that manufacturer's diagram rather than substituting B automatically.
Why the axial dimension letter matters: two separately checked catalog examples (mm)
The 15 mm inner-ring width of HR30205J is not its 16.25 mm assembled width. These examples are not added to the three-row deep-groove viewer above. NSK's boundary-dimension diagrams also distinguish radial width from thrust height.
C3 means internal clearance, not accuracy or a loose shaft fit
C3 means internal clearance, not accuracy or a loose shaft fit
Internal clearance is movement between a bearing's rings under the specified measuring conditions. A fit is the relationship between a ring and its shaft or housing seat. A precision class specifies dimensional and running accuracy. These are different quantities; see NSK's explanation of fits and clearance.
Selected NSK suffix meanings in the cited families
Suffix
Meaning
What it does not tell you
ZZ
Shields on both sides of the ball bearing
Not a load rating
DDU
Contact rubber seals on both sides
Not a universal seal code for every maker
VV
Non-contact rubber seals on both sides
Not the same sealing arrangement as DDU
C3
Radial internal clearance greater than CN, for the radial-bearing context shown
Neither a precision class nor a shaft/housing fit
P6
ISO tolerance class 6
Not an internal-clearance group
Prefixes matter too: NSK uses HR for its high-capacity tapered roller series. Read the complete maker-specific designation, including cage and lubrication details where required. Seals and shields affect exclusion of contaminants, friction and speed limits; they do not replace the catalog's load ratings. Sources: NSK TI/E/0111, auxiliary-symbol tables; NSK Bearing Designation Systems, sections 2 and 3.
Locate one end, allow thermal movement at the other, and distinguish end play from preload.
Locate the shaft at one end and allow growth at the other
Locate the shaft at one end and allow growth at the other
In a locating/non-locating arrangement, also called fixed/floating here, both supports carry radial load. The locating support also carries the applied axial load and establishes the shaft's axial position. The non-locating support allows axial movement as the shaft expands relative to the housing.
“Fixed” means axially located, not prevented from rotating. “Floating” means axial travel, not loose radial support.
Location needs a load path from shaft to bearing to housing: shoulders, suitable spacers, nuts, retaining rings or covers can retain the rings. Which end is fixed follows the required position of the driven parts; it is not automatically the left end or the motor end.
The floating end can accommodate movement inside a suitable bearing, such as an NU cylindrical roller bearing, or by controlled sliding of a ring in its seat. Do not loosen an arbitrary fit: see Tolerances and Fits and the bearing maker's mounting guidance.
Supporting detail: Addendum 61 — Why two locating supports can create unwanted load.
Keep shaft support separate from torque transmission. Bearings support the shaft relative to the housing; a keyed shaft-hub connection transfers torque to or from a pulley, sprocket or gear. Securing a hub against sliding along the shaft is a separate assembly requirement.
Heat the shaft and compare free travel with restraint; Interactive
Heat the shaft and compare free travel with restraint
Static comparison: at half the heating range, the shaft wants half the model's maximum free growth. A floating support with sufficient travel accommodates all of it. Two locating supports prevent it. With travel limited to 40%, half-range heating leaves 10% of maximum growth unaccommodated.
The drawing exaggerates growth. Heating level is a relative teaching scale, not a temperature or a material property. The left support and housing stay in place; only the shaft is heated. The dashed outline shows the length the shaft would reach if free. The solid outline shows the ideal constrained length. This model shows incompatible motion, not a binding force, stress or safe operating limit.
End play is free movement; preload is an initial internal load
End play is free movement; preload is an initial internal load
End play is the axial free movement available before the bearing arrangement takes up its clearance. Preload is a deliberately applied internal load before the external working load arrives. Reducing end play to a specified value and applying preload are different adjustments.
Do not tighten a bearing until it merely “feels solid.” Excess preload increases friction and temperature. Some arrangements require positive operating clearance; others use specified preload for stiffness or running accuracy. Temperature and fits change the operating condition.
A shim is a thin, accurately sized spacer. Changing its thickness sets a position in a rigid stack. Whether adding a shim increases or decreases end play depends on where the shim sits and which faces it separates.
Avoid burrs and rubbing contact that could release debris. Use the material and placement specified for the assembly.
A spring maintains force over travel; a shim sets distance; Checklist; Practice
A spring maintains force over travel; a shim sets distance
A shim sets distance and a spring maintains force.
A Belleville washer is a conical disc spring. A wave washer has an undulating shape that compresses axially. Both can apply preload when selected for the required force and working deflection.
A spring can accommodate small dimensional changes while maintaining load. “Very light load” is not a universal specification. Use the bearing's required preload and the spring's load-deflection data; an ordinary lock washer is not a calibrated preload spring.
Supporting detail: Addendum 62 — Position preload versus spring preload.
Identify which support locates the shaft and trace its axial load path.
Find where the other support permits thermal movement and check available travel.
Read the specified end play or preload and its measurement conditions.
Choose the prescribed shim or spring arrangement and verify the final measured setting.
Supporting detail: Addendum 63 — Manufacturer reading and open material questions.
Use the same degrees-of-freedom model to compare round shafts, profile rails and V-wheel carriages.
A linear guide leaves travel along one axis
A linear guide leaves travel along one axis
A linear bearing guides sliding motion just as a rotary bearing guides turning. Let x point along the travel. The guide supports transverse loads and, where its geometry allows, resists moments that would tilt or twist the carriage. A screw, belt or other actuator supplies travel force; the guide does not drive itself.
In the ideal model, translation along x is free. The desired constraints depend on whether rotation about x is acceptable. Real guide selection also checks load, moment capacity, stiffness, clearance, lubrication and alignment.
T means translation; R means rotation. “Restrained” assumes adequate bearing length or block spacing, engagement and rated loads. It does not mean infinite stiffness.
A round shaft does not provide an anti-rotation key
A round shaft does not provide an anti-rotation key
A plain round sleeve or linear ball bushing guides motion along a cylindrical shaft. In the ideal geometry it leaves two freedoms: Tx and Rx. The four other motions are restrained by the support's length or spaced bearings. A second parallel guide can stop the carriage rotating.
Geometric freedom is not a rotary service rating. A recirculating ball bushing may resist or wear under rotation even though its round shaft provides no positive anti-rotation feature. Use a product explicitly rated for combined linear and rotary motion when both are required.
LMU is a common catalog family label associated with round-shaft linear ball bushings. Treat it as a catalog name, not a universal standard or proof of rotary capability. Check the supplier's construction, dimensions and limits.
A profile rail constrains twist as well as sideways motion
A profile rail constrains twist as well as sideways motion
A shaped rail and matching carriage have separated contact paths that resist twisting and tipping. Within their moment ratings, they leave one degree of freedom: Tx. Mounting surfaces must keep the rail aligned; adding constraints can also make an assembly sensitive to misalignment.
MGN commonly identifies a miniature, narrow-block profile-guide family. For example, HIWIN uses MGN within its miniature MG series, with recirculating balls. The label does not make every supplier's product interchangeable, and does not describe every plain or roller guide.
Opposed V-wheels guide a carriage; one wheel does not; Practice
Opposed V-wheels guide a carriage; one wheel does not
A V-groove wheel runs on a matching edge or rail. A stable carriage commonly uses three or more wheels with contacts opposed across the rail and spaced along it. A triangular three-wheel arrangement can use an adjustable wheel to take up clearance.
The assembled carriage should leave only travel along the rail. Three wheels placed arbitrarily do not guarantee that result: orientation, spacing, contact retention and adjustment determine which loads and moments it can resist. A carriage that can lift away from its track has not constrained that motion.
Supporting detail: Addendum 64 — Manufacturer reading and the rotary-motion qualification.
The three quantities every schematic and nameplate uses, the units they are measured in, and the two equations that connect them.
Three quantities, three units
Three quantities, three units
Almost every electrical number you will read off a nameplate, a meter, or a
schematic is one of three quantities. Each has a name, a quantity symbol used in formulas, and a
unit symbol written after a value.
Current, I
The rate at which electric charge flows past a point.
Its unit is the ampere, symbol A — one of the seven SI base
units. One ampere is one coulomb of charge per second.
Voltage, V
Also called electric potential difference: the
difference in electric potential between two points. Its unit is the volt,
symbol V, defined as power per unit of current.
Resistance, R
How strongly something opposes the flow of current.
Its unit is the ohm, symbol Ω, defined as voltage per unit
of current.
How each unit is built out of the others.
Quantity
Unit
Symbol
In other units
Electric current
ampere
A
SI base unit; 1 A = 1 C/s
Electric charge
coulomb
C
s·A
Potential difference
volt
V
W/A, and so (N·m)/(A·s)
Resistance
ohm
Ω
V/A, and so W/A2
Say “amp” if you like; write A. The unit
name is the ampere, and the symbol is a capital A because the unit is named after a person. So is
the volt (V) and the watt (W). Lower case changes the meaning of a
prefix, not just the look of it: mA is a milliampere and MA is a
megaampere, a billion times larger. See Measurement Language.
Supporting detail: Addendum 65 — Why voltage and resistance are called derived units.
Two equations, and everything else follows
Two equations, and everything else follows
For an ohmic resistor (constant resistance under the stated conditions), the set is generated
by Ohm’s law and the power relationship:
V = IR — P = VI
Rearranging and substituting gives three expressions for each of the four quantities. There is
nothing to memorise beyond the two above; the table is a lookup, not a list of new facts.
Resistive-load magnitudes: steady DC, or RMS voltage and current for AC.
To find
From V and I or R
Using power
Using power
Voltage, V
V = IR
V = P/I
V = √(PR)
Current, I
I = V/R
I = P/V
I = √(P/R)
Resistance, R
R = V/I
R = V2/P
R = P/I2
Power, P
P = VI
P = I2R
P = V2/R
P = VI gives real power in watts on direct current or a purely
resistive load. For single-phase AC, RMS volts times RMS amps is apparent power in
volt-amperes, and the real power is that multiplied by the power factor — see
Power and Efficiency.
Worked example: what a lamp draws
Worked example: what a lamp draws
How much current does a 100 W resistive lamp draw on a 120 V supply (RMS for AC)?
Pick the form with the two quantities you have: I = P/V.
I = 100 W ÷ 120 V = 0.833 A.
Check the units rather than trusting the arithmetic. A volt is a watt per ampere, so watts
divided by volts leaves amperes — which is what was asked for.
Worked example: voltage drop along a cord
Worked example: voltage drop along a cord
A 100 ft extension cord has a total out-and-back conductor resistance of 0.1588 Ω.
What is the resistive voltage drop across that path when 10 A flows through it?
V = IR = 10 A × 0.1588 Ω = 1.588 V.
About 1.6 V. That is 1.6 V that never reaches the tool: for DC or an AC resistive load,
the supply voltage equals the cord drop plus the load voltage.
Supporting detail: Addendum 66 — The dropped voltage does not disappear.
The same method keeps working
The same method keeps working
These are not the last units you will meet. Each new quantity arrives the same way: it is
defined as a combination of quantities you already have, and its unit is that same combination.
A few more, and where each one comes from.
Quantity
Defined as
SI unit
Pressure or stress
Force per unit area
pascal, Pa = N/m2
Volumetric flow rate
Volume per unit time
m3/s
Specific weight
Weight per unit volume
N/m3
Capacitance
Charge per unit voltage
farad, F = C/V
Read the middle column and the right-hand column together and the pattern is the whole point:
the unit is the definition, written in symbols. Once that clicks, a unit you have
never seen tells you what the quantity is.
Sources
Sources
Supporting detail: Addendum 67 — Where these values were checked.
Engineering Fundamentals/Electrical Systems
AC and DC
Current direction, sine-wave voltage, transmission losses, and conversion between AC and DC.
DC flows one way; AC reverses direction
DC flows one way; AC reverses direction
Direct current (DC) flows in one direction. Its magnitude can change without making it AC. Alternating current (AC) reverses direction repeatedly. A battery supplies DC; a wall receptacle supplies AC.
Electronics generally run from a DC supply. That does not mean a transistor cannot handle an AC signal: transistors can amplify changing signals and act as switches. The supply and the signal are different parts of the story.
A 120 V sine wave peaks near positive and negative 170 V
A 120 V sine wave peaks near positive and negative 170 V
The nominal 120 V of a US receptacle is an RMS value: root mean square. For a sine wave, Vpeak = VRMS × √2, and VRMS = Vpeak / √2. Thus 120 × √2 = 169.7 V. The instantaneous voltage swings between about +170 V and −170 V, or about 340 V peak to peak.
Frequency counts complete cycles per second, in hertz (Hz). A 60 Hz waveform completes 60 whole cycles per second; a 50 Hz waveform completes 50. A cycle returns to the same phase, rather than ending at the opposite peak. US household mains is 60 Hz; many other countries use 50 Hz (DOE, Electricity 101).
Supporting detail: Addendum 68 — Why use RMS instead of the average voltage?.
Compare signed mean, RMS, and ideal-resistor heating; Interactive; Practice
Compare signed mean, RMS, and ideal-resistor heating
A sine can have a signed average of zero over one cycle and still produce heating. Add a DC offset and the
signed mean moves with the waveform, while total RMS combines the offset and the changing component. Predict
first, then compare the same sine centered on zero, shifted by an offset, kept above zero, or reduced to pure DC.
Print / static comparison: use the analytic waveform
v(t) = offset + amplitude × sin(2πft) over one complete cycle. The resistor is ideal and fixed at
100 Ω. These are low illustrative voltages, not mains or wiring examples.
The same 2 V sine amplitude with different DC offsets
Waveform
Signed mean
AC-component RMS
Total RMS
Minimum / maximum
Average resistor power
0 V offset
0 V
1.414 V
1.414 V
−2 / +2 V
20 mW
+1 V offset
+1 V
1.414 V
1.732 V
−1 / +3 V
30 mW
+3 V offset
+3 V
1.414 V
3.317 V
+1 / +5 V
110 mW
The centered sine has zero signed mean but nonzero RMS and average power. The +3 V offset keeps the total
waveform positive even though it still contains a sine component. A constant pure-DC value has RMS equal to
its magnitude and has no unique oscillation period.
The live explorer evaluates one complete ideal sine cycle analytically; the drawn points only illustrate the
equation. For v(t) = VDC + A sin(2πft), the signed mean is
VDC, the sine component has RMS A/√2, and total RMS is
√(VDC² + A²/2). In one ideal resistor, average power is
VRMS²/R; “RMS power” is not the quantity being calculated.
Higher transmission voltage reduces current and line loss
Higher transmission voltage reduces current and line loss
For the same transmitted power, a higher voltage allows a lower current. The line's resistive heating is Ploss = I2Rline. Halve the current and the loss becomes one quarter, if line resistance stays the same. Here Rline includes the complete current path.
Transformers made it practical to step AC voltage up for transmission and down for use. That advantage helped the AC systems associated with Westinghouse and Tesla prevail over Edison's early DC distribution system in the “war of the currents.” It was not one inventor winning every part of electrical engineering.
Supporting detail: Addendum 70 — A comparison with the same power and the same line.
A rectifier is one stage of an AC-to-DC power supply
A rectifier is one stage of an AC-to-DC power supply
A rectifier makes current flow in one direction from an AC input. Its output can still pulsate. Filtering smooths the output, and regulation controls the output voltage. A complete power supply may include all these functions as well as isolation.
Linear supply: commonly uses a line-frequency transformer, rectifier, filter, and linear regulator. The regulator dissipates excess voltage as heat.
Switch-mode supply: switches current rapidly and uses energy-storage components to convert voltage efficiently. An AC-input version also rectifies its input. Not every switch-mode converter provides isolation.
Both lose some input energy as heat. Efficiency depends on the design, input voltage and load; compare published efficiency curves at the intended operating point rather than assuming one percentage for a whole category. See Power and Efficiency for the input/output calculation.
An inverter makes AC from DC; the waveform matters
An inverter makes AC from DC; the waveform matters
A pure-sine inverter produces an output close to a sine wave. A modified-sine inverter produces a stepped approximation. Equipment may run differently, make more noise or heat, or fail to operate on a stepped waveform. Check the equipment manufacturer's compatibility guidance; equal RMS voltages do not make the waveforms interchangeable.
For grid-tied PV inverters, efficiency is typically above 95% under most operating conditions, according to Sandia PVPMC’s CEC Inverter Test Protocol. Efficiency depends on AC output power, DC voltage and sometimes temperature.
Every real conversion loses some energy. Several conversions in a row multiply their efficiencies rather than adding them. Much of what we use today runs on DC internally, even when it plugs into AC. Phones, computers, and microcontroller electronics bring the instructor's closing question into focus: who gets the last laugh?
Motors, generation, and energy storage make use of both forms of electrical power.
Engineering Fundamentals/Electrical Systems
Wire and Wire Gauge
Separate the conductor from its insulation, and understand what a wire gauge does and does not tell you.
The conductor carries current; insulation separates conductors
The conductor carries current; insulation separates conductors
The metal inside a wire is the conductor. Its resistance depends on material, length, cross-sectional area and temperature. The covering is insulation: it keeps the conductor from contacting other conductors or surrounding objects. The outside diameter includes that covering and does not by itself tell you how much metal is inside.
Solid wire has one solid conductor; stranded wire has several smaller strands forming a conductor. Insulation type and condition matter separately from the metal size. See Electrical Safety for use and inspection guidance.
A smaller AWG number means a thicker conductor
A smaller AWG number means a thicker conductor
American Wire Gauge (AWG) uses smaller numbers for larger conductor cross sections. For the same material, length and temperature, a thicker conductor has less resistance. See Adafruit’s wire-gauge explanation. Under comparable installation and temperature conditions, it can carry more current without exceeding its temperature limit.
Ampacity means the allowable current under specified conditions. Gauge alone is not an ampacity rating: material, insulation temperature rating, ambient temperature, bundling and installation all matter. Use the applicable manufacturer data and installation requirements for a real selection; this page is not a wire-sizing table. IEWC explains these ampacity factors. Choosing a wire involves voltage drop as well as allowable current.
Supporting detail: Addendum 71 — Why a long wire can matter even below its current limit.
Count the return wire: explore voltage drop and heating; Interactive; Practice
Count the return wire: explore voltage drop and heating
A two-conductor circuit carries current out and back. Use twice the one-way run for its wire resistance. At the same current, longer or thinner wire drops more voltage and wastes more power as heat. Voltage drop is a separate check from ampacity: get the current rating from the applicable code table or manufacturer for the insulation and installation.
Worked example: 50 ft out + 50 ft back = 30.48 m of copper. R = ρL/A = 0.6385 Ω. At 5 A, IR = 3.192 V and I²R = 15.96 W.
Voltage drop: baseline 3.192 V; now 6.385 VWire heating loss: baseline 15.96 W; now 63.85 W
Outline = baseline; filled = now. Each pair shares its own scale; compare within a pair. Loss is heating power, not wire temperature.
Doubling only current doubles the drop and quadruples heating loss. Doubling only length doubles both; a smaller AWG number lowers both at the same current.
This model assumes solid copper at 20 °C, equal outgoing and return wires, and DC/resistive behavior. Current is an input, not a prediction of how a particular load responds. Heating loss is not a temperature prediction; copper resistance rises with temperature (approx. 0.393%/°C near 20 °C). Connections and AC reactance are omitted.
Supporting detail: Addendum 72 — Definitions used to calculate every result.
Trace current paths, combine resistances, and explore how opening a switch changes voltage, current and power.
Series has one path; parallel has separate branches
Series has one path; parallel has separate branches
In a series circuit, the same current passes through every element. The voltage drops around the loop add up to the source voltage. One break stops current everywhere in that loop.
In a parallel circuit, each branch connects to the same two supply nodes (a node is an electrically connected junction), so each complete branch has the same voltage. The branch currents add up to the supply current. A break in one branch leaves the other branches working, provided the source and shared wiring remain intact.
Equal resistance gives equal drops in series and equal currents in parallel. Different resistances make the drops or currents different. The formulas for each individual resistor are on Current, Voltage, and Resistance.
Add resistances in series; add their reciprocals in parallel
Add resistances in series; add their reciprocals in parallel
Equivalent resistance is the single resistance that would draw the same total current at the supply terminals.
Series: Req = R1 + R2 + R3.
Parallel: 1/Req = 1/R1 + 1/R2 + 1/R3. A reciprocal is 1 ÷ R: one divided by the resistance. Include only connected branches.
Two parallel resistors: Req = R1R2 / (R1 + R2).
Check the result: series resistance is greater than any one positive resistor; parallel resistance is smaller than the smallest connected resistor when two or more branches are connected. An open circuit has no conducting path and is represented by infinite equivalent resistance.
Supporting detail: Addendum 73 — Why the parallel formula uses reciprocals.
Change a resistor or open a switch and predict what changes; Interactive
Change a resistor or open a switch and predict what changes
Use this ideal DC model to compare two or three fixed resistors. Before moving a control, predict which current, voltage and power will change. Switches are ideal, wires have zero resistance and the source holds its set voltage.
Static example: a 15 V source and 30 Ω and 60 Ω resistors, with both switches closed.
The same resistors in two connections
Connection
Equivalent resistance
Total current
R1: current / voltage / power
R2: current / voltage / power
Series
90 Ω
0.1667 A
0.1667 A / 5 V / 0.8333 W
0.1667 A / 10 V / 1.667 W
Parallel
20 Ω
0.75 A
0.5 A / 15 V / 7.5 W
0.25 A / 15 V / 3.75 W
Opening either series switch makes both resistor currents and both resistor voltage drops zero. Opening the R1 parallel switch makes R1 current and power zero while R2 still draws 0.25 A. The voltage across the whole open branch remains 15 V; it falls across the open switch, not the resistor.
The live table reports voltage across each resistor, excluding its switch. In an open series loop the source voltage is across the break or breaks. With several open switches, this ideal model does not determine how that voltage divides between the breaks.
Power explains the bulb comparison, within the model; Practice
Power explains the bulb comparison, within the model
For fixed resistors in series, the larger resistance dissipates more power because both carry the same current. In parallel, the smaller resistance dissipates more power because both have the same voltage. Check the power column rather than assuming the same bulb wins in both arrangements.
Greater electrical power is a useful brightness comparison for otherwise comparable incandescent bulbs. Real filaments change resistance as they heat, and LED lamps contain additional circuitry. The fixed-resistor model is not a universal lamp-brightness predictor.
Connect voltage, current, resistance and continuity measurements to the part of the circuit they describe.
Voltage is measured across; current is measured through
Voltage is measured across; current is measured through
A voltmeter measures the potential difference between two points. Connect it across the component, in parallel. A series ammeter becomes part of the current path: open the path and insert it in series with the element whose current you want.
A meter set for current has a low-resistance input; connecting that input across a source makes a short circuit. Read Electrical Safety before making physical measurements. The diagrams here explain connections, not a procedure for working on mains wiring.
Supporting detail: Addendum 74 — Real meters change the circuit a little.
Place both voltage probes, predict the sign, then reveal; Interactive; Practice
Place both voltage probes, predict the sign, then reveal
A DC voltmeter reports an ordered difference: V(red) − V(black). The two probes must touch the two named points you want to compare. Reversing them reverses the sign; putting both on the same conductor gives zero.
Static example: an ideal 12 V source supplies 30 Ω and 60 Ω resistors in series. Each resistor has an ideal switch immediately before it.
Signed readings from the same ideal circuit
Circuit state
Red point
Black point
Reading
Why
S1 open
Supply +
After S1
+12 V
The single open switch takes the source voltage; no current flows.
Both closed
After S1
After R1
+4 V
Current is 12/(30+60) = 0.1333 A; R1 drops 4 V.
Both closed, probes reversed
After R1
After S1
−4 V
The two point potentials are unchanged; only the ordered subtraction reverses.
S2 open
After R1
After S2
+12 V
The upstream side stays at +12 V and the downstream side returns to 0 V.
Any supported state
One named point
The same point
0 V
A point cannot have a potential difference from itself.
With two open switches, the conductor between them floats in this ideal model. Its voltage is not assigned. The interactive intentionally offers no two-open state.
This is a low-voltage ideal-circuit model with an infinite-impedance voltmeter. It does not authorize live work, mains measurements, or current-mode probing. Fluke's DC-voltage guide explains the V and COM inputs and the negative sign from reversed DC probes; its 381 meter manual shows that voltage probes touch the two desired test points.
A shunt or clamp lets you measure current indirectly
A shunt or clamp lets you measure current indirectly
A shunt is a known small resistance in the current path. Measure the voltage across it and use the relationship in Current, Voltage, and Resistance to find current. The shunt is in series; the voltage measurement across it is in parallel. Many ammeters contain a shunt internally. An installed shunt avoids opening the circuit each time you read it; adding one still requires changing the path.
A clamp meter senses the magnetic field around a conductor without breaking the circuit. Clamp around one conductor, not the outgoing and returning conductors together: their fields can cancel. The instrument must support the type of current being measured; an AC-only clamp does not measure steady DC.
Resistance and continuity are measured with the circuit unpowered
Resistance and continuity are measured with the circuit unpowered
An ohmmeter applies its own small test signal. Use it on an unpowered circuit, with stored energy discharged as described in Electrical Safety. Other connected paths can change the result; isolating the component lets you measure its resistance instead of the whole network.
Continuity is a resistance-threshold test. The beep means the measured resistance is below that meter's threshold. It does not prove exactly zero resistance, identify the intended path, or establish that a connection can carry its working current. The threshold comes from the meter's manual.
A multimeter combines voltage, current and resistance functions, often with continuity too. Select the function, AC or DC mode, range and lead sockets for the measurement. In a schematic, follow the actual connection points rather than the physical positions of the symbols.
Engineering Fundamentals/Electrical Systems
Electrical Diagram Types
Choose a drawing by the question it answers: appearance, connections, function, control logic, or physical location.
Choose the drawing for the job
Choose the drawing for the job
One electrical system can need several drawings. Start with the question: What does the part look like? Where does this wire go? How does the circuit work? Where does the equipment fit?
Choose the drawing for the question you need to answer.
Type
Shows
Usually leaves out
Who uses it, and when
Pictorial
Recognizable appearances of parts.
Exact electrical behavior and hidden connections may be omitted.
A beginner or assembler identifying parts before tracing connections.
Block
Functions and the direction of signal or power flow.
Individual terminals, component values, and return wires.
A designer explaining a system before working out its circuits.
Wiring
Connections between terminals; wire identifiers and routing where specified.
The reason the circuit behaves as it does; scale may be omitted.
An assembler or service technician connecting or tracing wires.
Schematic
Electrical function and connections using component symbols.
Actual component positions, wire lengths, and enclosure geometry.
A circuit designer or technician analyzing how a circuit works.
IC / PCB layout
Physical geometry: a PCB has footprints, pads and copper traces; an IC layout describes structures and interconnect on a chip.
A convenient explanation of circuit operation.
A board or chip designer checking placement and routing before manufacture.
Ladder
Relay or PLC control logic arranged in rungs between rails.
Exact equipment placement and wire routing.
A controls technician tracing the conditions for an output.
Logic
Gates and the relationships between logical inputs and outputs.
Power wiring, package pin locations, and physical placement unless added.
A digital designer following Boolean decisions through a circuit.
Electrical floor plan
Locations of outlets, switches and fixtures on a building plan, interpreted with its legend.
Internal circuit operation; complete routing may be on other drawings.
An installer or building designer locating devices within rooms.
Riser
Distribution between building levels and the equipment serving them.
Detailed room layouts and exact conduit paths unless specified.
A building electrical designer or installer coordinating distribution across floors.
Read the drawing title, legend, revision, and notes before treating a line or mark as an instruction. The same habit applies to mechanical drawings; see Choosing Drawing Views and The Alphabet of Lines.
Compare one circuit in pictorial, wiring, and schematic views; Interactive
Compare one circuit in pictorial, wiring, and schematic views
This teaching example connects a battery, switch, resistor, and LED in one loop. The resistor is in series with the LED. The drawings explain identity and connections; they do not specify a buildable parts list, resistor value, battery rating, or package pinout.
Choose a view. Choose a component to keep it marked when you change views.
Pictorial view
B1 batteryS1 switchR1 resistorD1 LEDRecognize the parts. These simplified silhouettes are not package dimensions or a lead-identification guide.
Wiring view
B1 battery−+S1 switch12R1 resistor21D1 LEDKAFollow terminals: B1+ → S1.1; S1.2 → R1.1; R1.2 → D1.A; D1.K → B1−. A means anode; K means cathode. Terminal names here belong to this example.
Schematic view
+B1 batteryS1 openR1 resistorD1 LEDCommon symbols preserve the wiring connections. S1 is shown open. The LED cathode is the bar on the battery-negative side; the outward arrows identify light emission.
Block view
B1 batterySupplies energyS1 switchControls the pathR1 resistorLimits currentD1 LEDProduces lightArrows show functional order, not individual conductors. The return conductor is omitted.
The wiring view retains every terminal connection. The block view deliberately removes that detail to explain each part's job. The schematic retains those connections while replacing part pictures with common symbols. Compare the three drawings together, or select one view to trace a part. On narrow screens the comparison stacks vertically.
A layout, floor plan, and riser answer different location questions
A layout, floor plan, and riser answer different location questions
A PCB footprint is the land pattern where a component attaches to a board. Traces are the board's conductive paths. An IC is a chip; its internal layout is not the same drawing as the board that holds it.
A floor plan places devices in rooms. Its legend tells you what each mark means. A riser makes the relationship between building levels easier to follow. Neither should be treated as a complete installation instruction by itself.
Read control logic without assuming physical placement
Read control logic without assuming physical placement
A ladder diagram arranges control conditions and outputs in horizontal rungs between two vertical rails. A relay drawing and a PLC program may use a similar ladder shape, but a PLC instruction tests a stored state; it is not a picture of a physical contact.
Common relay forms, shown with S1 open and K1 de-energized. Closing S1 energizes K1; its normally open contact closes and H1 lights. Opening S1 releases K1 and turns H1 off. The shared K1 label links the coil and its contact; it is not a wire between rungs. This is a functional example, not an installation drawing.
A logic diagram emphasizes operations such as AND, OR, and NOT. It helps answer which combinations of inputs produce an output. The diagram may omit supply connections and package pin numbers, so it does not replace a wiring drawing.
Continue with Reading Electrical Connections to recognize common component symbols, distinguish a joined wire from a crossing, and count electrical nodes.
Engineering Fundamentals/Electrical Systems
Reading Electrical Connections
Follow conductors and node labels instead of judging connections by where components sit on the page.
Read the connection convention before tracing a wire
Read the connection convention before tracing a wire
A schematic organizes electrical relationships, not the positions of parts on a bench. Stretching or bending a drawn wire does not change its connections. Moving a line onto a different terminal does.
For the examples on this page, a filled dot at a crossing means the wires join. A crossing with no dot means they do not join. Other drawings may use a bridge or different conventions. Check the legend; an unclear or damaged junction mark is a reason to consult the drawing source.
Count connected conductors, not corners or dots
Count connected conductors, not corners or dots
A node is a set of points joined by ideal conductors. Every point along an uninterrupted wire belongs to the same node, including its bends and branches. A dot marks a connection; it is not a separate component or an extra node.
In the figure, the dotted cross is one node. The undotted cross is two nodes: the horizontal conductor and the vertical conductor. This count concerns the wires drawn in the figure; no connection elsewhere is implied.
Do not trace through a resistor, diode, or open switch as if it were wire. If an ideal switch closes, its two sides become connected; state the switch position before counting nodes. Matching net labels can also indicate a connection without a continuous line across the page. Check the label scope and drawing notes before joining similarly named nets.
Read component identity separately from its value
Read component identity separately from its value
A reference such as R1 identifies a particular part; a value such as 1 kΩ describes its resistance. D1 can identify a diode or LED, so its symbol and parts information still matter. A ground label identifies a reference or connection according to the drawing; it does not by itself establish a connection to protective earth.
US practice (IEEE 315 / ANSI Y32.2) and international practice (IEC 60617) draw some symbols differently. Use the drawing legend; the forms below are teaching examples, not a claim of compliance with a standard.
Trace a connection one terminal at a time; Checklist; Practice
Trace a connection one terminal at a time
Read the legend, notes, revision, and stated switch positions.
Find the source and the named return or reference node.
Follow each conductor to a component terminal, junction, or net label.
Mark each uninterrupted group of conductors as one node.
Check crossings and similarly named labels before assuming they join.
Use the wiring drawing and parts documentation when physical terminal locations matter.
Recognize common symbols before tracing their connections; Practice
Recognize common symbols before tracing their connections
Use the symbol to identify the kind of component, then read its reference and value. The sheet includes both resistor forms and an unpolarized capacitor. A battery is one kind of DC source; other DC supplies may use a circle marked with polarity.
Common teaching forms, panel 1 of 2.
Common teaching forms, panel 2 of 2. Buzzer and fuse shapes vary, so check the legend. The ground mark's meaning depends on the drawing; it does not establish protective earth by itself. The diode bar marks its cathode; the LED adds outward arrows for light.
Find the stator and rotor, then follow the changing magnetic field that keeps a motor turning.
The stator stays still; the rotor turns
The stator stays still; the rotor turns
An electric motor turns electrical input into mechanical motion. In a rotary motor, the stator is the stationary part and the rotor is the rotating part. An air gap separates them. Bearings support the rotating assembly; the shaft carries motion to the load.
The stator is often outside the rotor, but it does not have to be. The names describe motion, not inside versus outside. See Electric Motor Types for both arrangements.
Keep the magnetic target moving: carrot on a stick
Keep the magnetic target moving: carrot on a stick
Picture the rotor turning to align its magnetic field with the stator's field. If the fields simply settled into alignment, that turning effect would disappear. To keep turning, the motor switches a field or keeps the stator field rotating. Think carrot on a stick: keep moving the target ahead.
Commutation means switching current between windings at the right time. Brushes and a commutator can do it mechanically, or a drive can do it electronically. A winding is a coil of wire that creates a magnetic field when current flows through it.
Supporting detail: Addendum 76 — Where the alignment picture needs care.
Why a DC motor keeps turning: coil, field and commutator; Interactive
Why a DC motor keeps turning: coil, field and commutator
The simplest brushed DC motor is one rectangular coil on a shaft between two magnet poles. Turn the coil, find where the field stops pushing it, and see how a split-ring commutator keeps the push going one way.
Predict first: a coil carrying current sits between a north and a south pole. At which angles does the field give it no turning push at all, and where is the push largest?
Torque on the coil. For an ideal rectangular coil in a uniform field, the torque about the shaft is τ = N·B·I·A·sin θ. N is the number of turns, B the field (T), I the current (A) and A the coil's area (m²), so τ is in N·m. θ is the angle from the field B to the coil's normal n, the line perpendicular to the coil's face. The coil's magnetic moment lies along n or against it, depending on which way the current circulates. That sets the direction of the torque, not its size.
One coil at θ = 30°. Left, a cutaway side view: the N pole in front is cut away, the S pole is behind the coil, and B points away from you. Right, the end view from the commutator end, with the top brush positive. In the end view, current runs away from you along side 1 (⊗) and back toward you along side 2 (⊙). F = BIL pushes side 1 down and side 2 up. The two forces are equal and opposite, so there is no net force, but they form a couple. Each acts at a lever arm of r·sin 30° = 0.5r from the shaft, where r is half the coil width. So τ = 0.5·NBIA, counter-clockwise as seen from the commutator end.
Why the angle matters. Whenever current flows, each long side of the coil feels a force F = BIL, the same size at every angle. What changes is its lever arm about the shaft, r·sin θ, where r is half the coil's width. As the coil approaches θ = 0° or 180°, with its face across the field in the neutral plane, the forces point almost straight through the shaft. The lever arm shrinks to zero, and so does the torque. With slip rings the current still flows at those angles and the forces point straight through the shaft. With an ideal split ring the brushes sit on the gaps at that instant, so there is momentarily no current and no force at all. Either way the torque there is zero. At θ = 90° and 270° the lever arm, and the torque, are largest.
Why a commutator. If the coil were fed through slip rings, its current would never reverse. With the polarity drawn here, past 180° the torque would reverse too, pushing the coil back toward that neutral-plane position, and over a whole turn it would average zero. Reverse the supply or the magnets and the coil's resting position moves half a turn. A split-ring commutator turns with the coil. Its brushes change segments exactly as the coil crosses the neutral plane, which reverses the coil current. The torque becomes N·B·I·A·|sin θ|: it never points backward, but it still falls to zero twice a turn.
0°90°180°270°360°10−11.41Torque ÷ one coil’s peak NBIAθ, angle from B to the coil normal ntwo coils (thick)one coil, commutatorone coil, slip rings (dashed)zeroTorque against θ for one turn, as a fraction of one coil’s peak NBIA. Slip rings (dashed): the torque reverses every half turn and averages zero. Split-ring commutator (solid): the current reverses at the neutral plane, so the torque is |sin θ|, never negative, averaging 2/π ≈ 0.64; it is still zero at 0° and 180°. Two commutated coils 90° apart (thick): the sum runs from 1 to √2 ≈ 1.41, so the smallest torque is 0.71 of the largest and never zero.
Two coils. Add a second coil 90° ahead of the first, each with its own split ring. When one coil is in the neutral plane, the other is at its peak. The total, |sin θ| + |cos θ| in units of one coil's peak, runs from 1 to √2. Its smallest value is 1/√2 ≈ 0.71 of its largest, so the ripple shrinks and the zero-torque dead spot disappears.
Worked example, with illustrative numbers rather than a real motor rating: N = 50 turns, B = 0.20 T, I = 2.0 A, and a coil 40 mm × 30 mm, so A = 1.2 × 10⁻³ m². The peak torque is N·B·I·A = 50 × 0.20 × 2.0 × 0.0012 = 0.024 N·m. At θ = 30°, τ = 0.024 × sin 30° = 0.012 N·m.
Direction. Reversing the current reverses every force (F = I L × B), so the motor turns the other way. Swapping the magnets reverses B and does the same. Reversing both restores the original direction.
Model limits. This is an ideal teaching model: one or two rectangular coils, a uniform field, and current switched exactly at the neutral plane. Torque is shown as a fraction of one coil's peak, N·B·I·A. It does not model back EMF, speed, magnetic saturation or brush sparking.
Supporting detail: Addendum 77 — Sources for the torque formula and the commutator.
Separate turning effort, speed, and power
Separate turning effort, speed, and power
Torque is turning effort. Angular speed tells how fast the shaft turns. Mechanical power combines the two. A stopped shaft can have torque and still deliver zero mechanical power.
Compare how motors switch their fields, what wears, and how they control motion.
Brushed DC: simple supply, wearing contacts
Brushed DC: simple supply, wearing contacts
A small permanent-magnet brushed DC motor has stationary magnets and rotating electromagnets. Carbon brushes press against a segmented copper commutator. As the segments rotate past the brushes, the connections change and reverse current in rotor windings. The torque keeps acting in the intended direction.
Strength: inexpensive and simple to run from DC, useful in small toys, pumps, and actuators. Weak points: brushes wear through contact and electrical arcing; the commutator and spring contact system can also deteriorate. Switching current at the contacts can cause sparks and electrical noise. Permanent-magnet construction is common in small motors; some brushed motors use field windings instead.
A microcontroller can command a power driver with pulse-width modulation (PWM), switching the supply on and off rapidly to control the motor. The driver handles motor current; a logic output is not a motor power supply.
AC induction: the rotor follows a rotating field with slip
AC induction: the rotor follows a rotating field with slip
Stator windings arranged around the motor produce a rotating magnetic field. In a three-phase motor, the currents reach their peaks at different times, moving the combined field around the stator. That moving field induces current in conducting rotor bars. The rotor current and stator field interact to produce torque.
The rotor runs slightly slower than the field during normal motoring. The difference is called slip. If the rotor caught the field exactly, there would be no relative motion to induce the rotor current needed for torque. For example, a field at 1,800 rpm and a rotor at 1,740 rpm differ by 60 rpm, or 3.33% of field speed.
Strength: a squirrel-cage induction rotor needs neither brushes nor permanent magnets, making it useful for pumps, fans, and conveyors. Weak points: speed changes with load and slip; a variable-frequency drive is normally used when adjustable speed is needed.
Supporting detail: Addendum 78 — Why alternating current alone is not the full explanation.
Brushless permanent-magnet motors: switch the stator current
Brushless permanent-magnet motors: switch the stator current
Here the rotor carries permanent magnets and the stator carries windings. A drive switches the stator currents in sequence so the magnetic field turns. There are no commutator brushes to wear.
BLDC means brushless DC; PMSM means permanent-magnet synchronous motor. A DC supply can feed an inverter, an electronic circuit that creates changing phase currents. Most BLDC/PMSM drive systems use this electronic switching. The labels often distinguish waveform and control choices; they do not mean one rotor needs AC magnets and the other needs DC magnets.
A suitably designed line-fed synchronous motor instead follows a rotating field set by the AC supply frequency and pole count. It needs an appropriate starting arrangement. Do not assume an arbitrary BLDC motor can connect directly to an AC line.
Strengths: no brush contact wear and controllable speed; common uses include cooling fans, drones, and controlled machine drives. Weak points: drive electronics and correctly timed switching are needed; bearings still wear and winding temperature still limits output.
Inner-rotor and outer-rotor describe what rotates
Inner-rotor and outer-rotor describe what rotates
An inner-rotor motor, also called an inrunner, rotates inside the stator. An outer-rotor motor, or outrunner, rotates around the stator. These are the arrangements sometimes called “inboard” and “outboard.” Use inner-/outer-rotor when describing the construction.
An inner rotor can have low rotational inertia, useful for rapid speed changes. An outer rotor puts magnetic force at a larger radius, useful for producing torque in fan and propeller drives, but its rotating shell contributes inertia. Dimensions and design still decide the actual performance.
Stepper: count commanded steps, but allow for missed motion; Practice
Stepper: count commanded steps, but allow for missed motion
A stepper drive energizes stator phases in a sequence of magnetic positions. As a first approximation, picture an inner-rotor brushless motor with many magnetic poles or teeth. That helps explain the small steps; it is a simplification, since stepper constructions differ.
Open loop means the controller sends a move without measuring whether it happened. A stepper can position and hold without feedback while energized and within its torque capability. It is useful for printer axes and small indexing mechanisms. Holding position still uses current and produces heat.
The weak point is missed steps. Excessive load or acceleration can prevent commanded motion. Without feedback, the controller keeps counting commands and does not know the shaft fell behind. Step count is not a guarantee of exact position, and holding torque is not a guarantee against any load.
A servo is a motor used with feedback and closed-loop control, not one particular magnetic construction. A sensor such as an encoder measures motion. The controller compares measured position or speed with the command and adjusts the drive to reduce the error.
Strength: responds to a load disturbance and detects position error, useful for robot joints and machine axes. Weak points: adds sensor, controller, tuning, and cost. Feedback does not create extra torque; a servo can still reach its limits. A brushed, brushless, or other suitable motor can be part of a servo system.
Linear motors move directly along a track
Linear motors move directly along a track
Think of the magnetic layout of a rotary motor opened out into a straight line. A traveling field pushes or pulls a moving member along a track, producing linear force instead of shaft torque. One permanent-magnet arrangement uses a magnet track and a moving coil assembly. Linear induction designs also exist; a magnetized rail is not universal.
Strength: direct linear motion without a rotary-to-linear screw or belt, useful for positioning stages and transport systems. Weak points: the magnetic track, drive, cooling, and position measurement can add cost. Separate guides support and constrain the moving assembly; a motor does not replace the guide system.
Use an ideal linear torque-speed curve to find a load point and see why peak output power occurs halfway to no-load speed.
More load torque means less speed on this curve
More load torque means less speed on this curve
This model approximates a permanent-magnet DC motor at a fixed supply voltage with a straight line between two endpoints. Stall torque is the torque at zero speed. No-load speed is the speed at zero external shaft load. It is not a universal curve for induction motors, steppers, or regulated drives.
Let Ts be stall torque, n0 no-load speed, and T the constant resisting load torque. The steady operating point is where motor torque equals load torque:
n = n0(1 − T/Ts).
This is an assumed linear approximation, not a measured motor rating. It omits acceleration, current limiting, temperature changes, and supply voltage drop. At stall it predicts zero shaft power, not zero electrical input. A stall rating is not a continuous operating rating.
Supporting detail: Addendum 79 — Manufacturer basis for the straight line.
Explore the load point and the peak-power point; Interactive
Explore the load point and the peak-power point
Predict first: a model motor has 0.8 N·m stall torque and 3,000 rpm no-load speed. A constant load asks for 0.2 N·m. Does the motor run above or below half speed?
Static example: n = 3,000(1 − 0.2/0.8) = 2,250 rpm. Angular speed is 2,250 × 2π/60 = 235.6 rad/s, so output power is 47.12 W. Peak power is 62.83 W at 1,500 rpm and 0.4 N·m.
The solid line is torque / stall torque; the dashed curve is power / peak power. The circle marks load torque; the diamond marks output power. The square marks peak power.
Peak power is halfway, not at either endpoint; Practice
Peak power is halfway, not at either endpoint
Use P = Tω, with torque in N·m and angular speed in rad/s. Convert rpm using ω = 2πn/60. The definitions and units are on Power and Efficiency and Angular Motion.
At stall there is torque but no speed. At no load there is speed but no external load torque. Both endpoints therefore have zero shaft output power. Between them, torque times speed reaches a maximum.
Supporting detail: Addendum 80 — Derive the halfway result from the straight line.
Supporting detail: Addendum 81 — Manufacturer check on peak power.
Peak efficiency needs electrical input as well as shaft output
Peak efficiency needs electrical input as well as shaft output
Efficiency is output power divided by input power. Peak output power and peak efficiency answer different questions. The torque-speed line alone does not give electrical input or losses, so this explorer deliberately does not calculate efficiency.
For the brushed coreless DC motors described by Portescap, peak efficiency occurs at a lighter load and higher speed than peak output power. Its exact position needs loss or current data. No external load means no useful shaft output, even though a real motor draws current to overcome its internal losses. Consult the actual motor's efficiency and continuous-operation data before selecting a load point.
Supporting detail: Addendum 82 — Manufacturer basis for the efficiency comparison.
Match the motor, reduction, and the same output load; Interactive; Practice
Match the motor, reduction, and the same output load
A gearbox changes the torque demanded at the motor shaft for the same output load. That can move the motor to a different point on its torque–speed curve. Predict both operating points before revealing them.
Static example: a motor has 0.8 N·m stall torque and 120 rpm no-load speed. The output load resists with 0.6 N·m. Compare direct drive with a 20-tooth driver, 40-tooth driven gear, and a stated 90% running mesh efficiency.
The same motor and output load, two connections
Connection
Torque required at motor
Motor speed
Output speed
Motor shaft power
Modeled output power
Direct
0.600 N·m
30.0 rpm
30.0 rpm
1.885 W
1.885 W
2:1 reduction, 90%
0.3333 N·m
70.0 rpm
35.0 rpm
2.443 W
2.199 W
Result: the reduction runs the output faster under this load, even though it divides motor speed. It reflects less load torque to the motor, so the motor reaches a higher speed. The gearbox did not create power: motor shaft power changed before the 10% modeled mesh loss.
This is a fixed-voltage steady-running comparison with a constant resisting torque. It does not establish starting ability, acceleration, thermal or continuous rating, back-driving, electrical input, or gear strength. At stall, speed and shaft output power are zero; if required motor torque exceeds stall torque, the model reports no forward steady operating point instead of assigning a fictitious speed.
Supporting detail: Addendum 83 — Source and the standstill boundary.
Real loads may demand different torque at different speeds. Their operating point is an intersection of a load curve and a motor curve. Practice reflected loadPractice output power
Engineering Fundamentals/Electrical Systems
Microcontroller Basics
Read inputs, make decisions in a program, and control outputs using a classic Arduino Uno R3.
A microcontroller reads inputs and controls outputs
A microcontroller reads inputs and controls outputs
A microcontroller is a small computer on a chip, with a processor, memory and connections to the outside world. Its program can read a switch, decide what that input means, and turn an output on or off. The Arduino Uno is a board that supplies the chip with power connections, a USB interface and accessible pins.
This topic uses the classic Uno R3 with an ATmega328P, operating with 5 V logic. Other Arduino boards, including newer Uno models, can have different converters and electrical limits.
An Arduino program is called a sketch. It uses C/C++ syntax: rules for names, parentheses, braces and statements. It is a programming language, not ordinary English. Capitalization matters: digitalRead and digitalread are different names.
setup() runs once after startup or reset. loop() repeats while the program runs. This original example turns the built-in LED on for half a second and off for half a second.
delay uses milliseconds and pauses normal progress through the sketch. The braces group the statements belonging to each function.
Choose the pin mode before using the pin
Choose the pin mode before using the pin
Three pin modes
Mode
What it does
Typical use
INPUT
Reads a voltage level without enabling the internal pull-up.
A sensor that actively drives a compatible signal; do not leave the input floating.
OUTPUT
Drives the pin HIGH or LOW.
An LED through a current-limiting resistor, or a control signal to a driver.
INPUT_PULLUP
Reads an input with an internal resistor pulling it toward the logic supply.
A button connecting the input to ground.
pinMode(pin, mode) configures the pin. digitalRead(pin) returns HIGH or LOW. On an OUTPUT pin, digitalWrite(pin, HIGH) drives it toward the logic supply; LOW drives it toward ground. These are limited-current signals, not ideal power supplies. On an INPUT pin, digitalWrite instead controls the pull-up.
A button to ground reads LOW when pressed
A button to ground reads LOW when pressed
With INPUT_PULLUP, an open switch reads HIGH. Closing the switch to ground reads LOW. This is called active-low: the action happens when the signal is low.
The pull-up supplies a small current through the closed switch to ground. The switch sinks that current. A physical switch can bounce between states briefly; counting presses reliably needs debouncing beyond this simple state display.
Supporting detail: Addendum 84 — Pull-up resistance and current.
Use the official IDE and function reference; Checklist; Practice
Confirm the board model and choose its matching board entry in the IDE.
Select the port belonging to the connected board.
Verify the sketch to catch syntax errors, then upload it.
Check that the observed input and output match the program.
Disconnect power before changing wiring. Keep signals within the board's ratings and use a suitable driver for a motor. See Electrical Safety for electrical precautions.
Decide whether a sensor communicates with two logic states, a changing voltage, or the timing of pulses.
Digital uses two states; analog uses a range
Digital uses two states; analog uses a range
A digital input interprets two states: LOW/HIGH, or 0/1. The wire still carries a physical voltage; the receiving circuit decides which logic state it represents. A voltage in the undefined region between valid LOW and HIGH levels is not a useful third state.
An analog signal represents a quantity by a continuous range of values. A potentiometer wired between ground and 5 V can provide a changing voltage at its middle terminal. On a classic Uno R3, the usual analog measurement range is nominally 0–5 V with the default reference. That is not a universal sensor range.
Classify the sensor's output circuit, not just its name
Classify the sensor's output circuit, not just its name
Common examples
Device and connection
Signal at the input
Button or switch with a pull-up
Digital open/closed state.
Quadrature encoder with compatible logic outputs
Two digital pulse trains; their order gives direction.
HC-SR04 ultrasonic module, Echo pin
A timed digital pulse. Its duration represents distance; its voltage height does not.
Potentiometer connected as a voltage divider
Analog voltage from its wiper (middle terminal).
Photoresistor in a voltage divider
Analog voltage as resistance changes with light.
Phototransistor with a load resistor
Analog response to light unless a threshold circuit converts it to digital.
Pressure or proximity sensor
Depends on the model: analog voltage, switching output, or digital data. Read its documentation.
A bare resistive sensor does not generate a usable voltage by itself: its surrounding circuit matters. A module may offer both analog and thresholded digital outputs.
Supporting detail: Addendum 85 — Phototransistor circuits can measure light or switch at a threshold.
Supporting detail: Addendum 86 — Why an ultrasonic measurement can be digital.
The ADC reads voltage; PWM controls time; Practice
The ADC reads voltage; PWM controls time
Analog-to-Digital Conversion turns an analog input into a number the program can use. Pulse-Width Modulation switches a digital output on and off for a controlled fraction of each cycle. Neither operation changes the fact that the processor stores and works with digital data.
Relate an Uno R3's 10-bit ADC reading to its reference voltage, step size and approximate sampling time.
Ten bits give 1024 codes, numbered 0 through 1023
Ten bits give 1024 codes, numbered 0 through 1023
An analog-to-digital converter (ADC) samples a voltage and reports a number. The classic Uno R3 has a 10-bit ADC: 210 = 1024 possible codes. analogRead(A0) reads analog input A0 and returns an integer from 0 to 1023.
The reference voltage sets the scale. With an assumed exact 5.000 V reference, one nominal step is 5/1024 = 0.0048828125 V = 4.883 mV, or about 4.9 mV. Resolution describes the step size; it does not guarantee that a real voltage measurement is accurate to that amount.
Supporting detail: Addendum 87 — Arduino's resolution and timing figures.
Use 1024 for the nominal voltage step
Use 1024 for the nominal voltage step
For these exercises, use a clearly defined ideal bin model: divide the 0–5 V span into 1024 equal bins, round down to the bin number, and limit the top code to 1023.
code = min(1023, floor(Vin × 1024 / Vref)). Here floor means round down. At 3.000 V with a 5.000 V reference: floor(614.4) = 614.
To report the nominal voltage represented by a code, use its lower bin edge: V = code × Vref/1024. Code 800 represents 800 × 5/1024 = 3.90625 V. In this model its bin extends up to, but not including, 3.9111328125 V.
Supporting detail: Addendum 88 — Why dividing by 1023 answers a different question.
Explore the steps and check the units; Practice
Explore the steps and check the units
The two-way ADC controls in the PWM and ADC explorer let you enter a voltage or a code. Try nearby voltages within one bin, then cross its boundary. In reverse, code 1023 gives 4.9951171875 V as its lower edge, not proof that the input equals that value.
The same explorer also separates when a voltage is sampled from how its code is calculated. It shows instantaneous raw PWM or settled RC values, the finite mean of the selected point samples, and the mean of their reconstructed lower-edge voltages. Those are different from the waveform's complete-cycle time mean. A held code is the latest point result, not a window average.
Supporting detail: Addendum 89 — Quantize first or average first?.
Explore duty cycle, frequency, average voltage and RC smoothing, then compare PWM output with ADC input.
Duty cycle is the fraction of each cycle spent HIGH
Duty cycle is the fraction of each cycle spent HIGH
Pulse-width modulation (PWM) repeats a rectangular waveform. The period T is the time for one cycle; frequency f is cycles per second. Duty cycle D is the fraction of the period spent HIGH.
T = 1/f, ton = D × T, and for ideal switching between 0 V and a supply Vs, Vaverage = D × Vs. Convert a percentage to a fraction: 25% means D = 0.25.
At 500 Hz, T = 0.002 s = 2 ms = 2000 µs. At 25% duty, the on-time is 500 µs and the average of a 0–5 V output is 1.25 V. The pin itself still switches between 0 and 5 V.
The stock Uno R3 uses six PWM pins
The stock Uno R3 uses six PWM pins
Use digital pins 3, 5, 6, 9, 10 and 11. Default PWM is approximately 490 Hz on 3, 9, 10 and 11, and 980 Hz on 5 and 6. These correspond to periods of about 2.04 ms and 1.02 ms.
analogWrite(pin, value) requests duty using values from 0 (always off) to 255 (always on). A useful nominal mapping is value = round(255 × D): 25% gives 64. Hardware timer modes introduce small differences in the exact duty, particularly near the ends of the range.
Supporting detail: Addendum 90 — Official frequency table and timer limitations.
Change duty and frequency, then compare an ADC reading; Interactive
Change duty and frequency, then compare an ADC reading
Print / static comparison: 25% duty at 500 Hz gives a 2 ms period, 0.5 ms HIGH time and a 1.25 V complete-cycle time mean for an ideal 0–5 V waveform. A point sample is one instant, not that average.
The same PWM waveform sampled at different phases
Finite sample set
Each raw sample
Selected-sample mean
ADC code / lower edge
500 samples/s, phase 10%
5 V
5 V
1023 / 4.995117 V
500 samples/s, phase 60%
0 V
0 V
0 / 0 V
2000 samples/s, phases 1%, 26%, 51%, 76%
5, 0, 0, 0 V
1.25 V
Mean lower edge 1.248779 V
An unloaded 10 kΩ / 1 µF RC filter has a 10 ms time constant. In the settled repeating response its 25%, 500 Hz ripple runs from about 1.1579 V to 1.3453 V while its cycle mean remains 1.25 V. Changing a control recomputes that settled response; this model does not show startup.
With a separate 5.000 V ADC input, 3.000 V gives code 614; code 800 has lower edge 3.90625 V.
The explorer is a model, not a board connection. Its frequency and sampling controls do not configure an Uno or claim a board throughput. A raw sample uses normalized phase with HIGH on [0, D) and LOW on [D, 1); the stated finite sample count defines the reported sample mean. ADC controls use the ideal bin convention on Analog-to-Digital Conversion; 5.000 V is assumed exact.
Supporting detail: Addendum 91 — Why more samples can still give the wrong mean.
An RC filter smooths PWM but leaves ripple
An RC filter smooths PWM but leaves ripple
Put a resistor in series with the PWM signal and a capacitor from the output node to ground; measure the voltage across the capacitor. This RC low-pass filter slows voltage changes. The capacitor charges while PWM is HIGH and discharges while it is LOW.
The time constant is τ = R × C. A longer time constant relative to the PWM period reduces ripple but makes the output respond more slowly when duty changes. The explorer shows the settled waveform with τ = 10 ms, assuming an ideal source and no load. A load changes the result; the filter is not a motor power supply.
Microchip's AVR131 PWM filtering note explains the tradeoff: the low-pass filter must reject PWM base-frequency ripple without removing the slower signal of interest, and a low-impedance load can discharge the capacitor unless buffered. This explorer deliberately assumes no load.
Supporting detail: Addendum 92 — What the smoothed trace calculates.
PWM changes LED brightness and motor drive; Practice
PWM changes LED brightness and motor drive
Rapid switching changes an LED's average light output while a resistor or driver limits its on-state current. Perceived brightness is not perfectly proportional to duty. For a DC motor, PWM commands a suitable power driver; the board pin does not supply the motor current. The driver must handle the motor and its inductive current.
Increasing duty usually increases the available drive, but motor speed also depends on load. Use DC Motor Torque, Speed, and Power to connect speed, torque and current. See Electrical Safety before wiring.
How turbines and generators turn other forms of energy into electricity, how photovoltaics differ, and how to compare a generation mix.
A generator converts motion into electrical energy
A generator converts motion into electrical energy
A generator does not create energy. It takes mechanical work at a shaft and delivers electrical energy to a circuit, with some energy becoming heat along the way.
A turbine is a rotating machine driven by a moving fluid. Steam, flowing water, wind, or hot combustion gases can turn its blades. The turbine turns the generator; the generator supplies electricity. An engine can also drive a generator without a turbine.
Supporting detail: Addendum 93 — How rotation produces electricity.
Different heat sources can feed the same steam cycle
Different heat sources can feed the same steam cycle
Burning fossil fuels or biomass can heat water to make steam. Nuclear fission supplies heat without combustion. Geothermal systems use heat from the Earth, and concentrated solar systems use mirrors to collect sunlight as heat. The equipment differs, but a steam-based plant follows the same basic chain: heat, moving steam, shaft rotation, electricity.
Not every turbine uses steam. A hydroelectric turbine takes energy from water flowing downhill. A wind turbine takes energy from moving air. A combustion turbine uses hot gases directly; a combined-cycle plant also recovers exhaust heat for a steam cycle.
Photovoltaic cells skip the turbine
Photovoltaic cells skip the turbine
A photovoltaic (PV) cell converts light directly into electrical energy through the photovoltaic effect in a semiconductor. A connected load receives DC electricity. An inverter can convert that DC to AC.
Solar PV and concentrated solar thermal are different routes. PV produces electricity in the cell; solar thermal first collects heat. That distinction matters when considering thermal storage.
A generation mix is more than a list of percentages
A generation mix is more than a list of percentages
A generation mix describes how much electricity comes from each source over a stated place and time. Installed capacity describes how much power equipment is rated to supply. Those are different measures: a large rated capacity does not mean a source supplied the same share of annual energy.
Predict: which generator produces more energy?
Compare two hypothetical generators over the same 365-day, 8760-hour period. Generator A is rated at 1 MW with a given 25% capacity factor. Generator B is rated at 0.5 MW with a given 60% capacity factor. Which produces more energy over the year? Decide before opening the check.
Check the rated-power and period-energy comparison
Period energy = rated power × period hours × capacity factor Capacity factor = period energy ÷ (rated power × period hours)
Fixed stated ratings and given illustrative factors over 8760 hours
Generator
Rated power
Capacity factor
Average power
Period energy
A
1 MW
25% = 0.25
0.25 MW
1 × 8760 × 0.25 = 2190 MWh
B
0.5 MW
60% = 0.60
0.30 MW
0.5 × 8760 × 0.60 = 2628 MWh
Generator B has the smaller rating but produces more energy in this given example. MW measures power; MWh measures energy over time. Do not treat 1 MW as 1 MWh for the year, and write 25% as 0.25 in the multiplication, not 25.
Capacity factor is not conversion efficiency, the percentage of hours switched on, dispatchability, reliability, or a source's share of an energy mix. Partial-load operation contributes too; the factor does not require a generator to alternate only between off and full power.
These ratings and factors are fixed hypothetical inputs for the stated period, not real-plant data. EIA's published factors use time-adjusted capacity methods; this example does not reproduce that method. The EIA capacity and generation FAQ distinguishes rated power from energy produced over a period and defines the capacity-factor comparison.
Compare cost, emissions, variability, and dispatchability — the ability to adjust output when requested. Wind and sunlight vary with weather and time. Fuelled generation and reservoir hydro can often be scheduled, but fuel, water, maintenance and operating limits still matter. Storage shifts energy in time; it is not an extra primary energy source.
No current percentage mix is supplied here. For dated U.S. generation data, consult the U.S. EIA's Electricity explained: electricity in the United States, and record the reporting year and whether the figures describe generation or capacity.
Engineering Fundamentals/Electrical Systems
Energy Storage Methods
Pumped water, stored heat and rechargeable batteries hold energy for later use in different ways.
Pumped hydro stores energy by lifting water
Pumped hydro stores energy by lifting water
Use electricity to pump water uphill, then let it flow downhill through a turbine and generator when electricity is needed. The stored energy is gravitational potential energy.
The cycle returns less electrical energy than it consumed because pumping, flow and generation all have losses. It needs suitable elevations, reservoirs and water management; it cannot be placed wherever a battery can.
Thermal storage holds energy in a hot material, such as a fluid or solid. A concentrated solar plant can collect heat while sunlight is available, store it, and later use it to produce steam and electricity. Stored heat can also serve heating loads directly.
Insulation slows heat loss; it does not eliminate it. Returning heat to electricity adds conversion losses. Choose the storage route for the energy form the load needs.
Rechargeable batteries store energy chemically
Rechargeable batteries store energy chemically
A battery supplies DC through electrochemical reactions. A primary battery is intended for a single discharge life and replacement. A secondary battery is designed to be recharged with a suitable charger, restoring chemical energy for another discharge.
Primary cells are useful portable energy supplies, but they are not reusable storage for electricity from a generator. Do not try to recharge a primary cell. Rechargeable does not mean unlimited life: cycling and aging reduce usable capacity.
Choose storage for the load and the site; Practice
Choose storage for the load and the site
A small portable instrument needs a compact energy supply, so a battery is a practical fit. A site with suitable upper and lower reservoirs can consider pumped hydro for large stationary storage. A solar thermal plant needing heat after sunset can store heat without first converting it to electricity.
Compare the required power, the energy needed over time, the storage duration, available space and terrain, losses, and service life. These examples identify a good fit; they do not establish that one technology is always cheapest.
Compare primary alkaline, rechargeable nickel, lead-acid and lithium-ion batteries, and the short history behind them.
Capacity, self-discharge and aging are different
Capacity, self-discharge and aging are different
A cell is one electrochemical unit. A battery may contain one cell or several. Its chemistry helps determine voltage, mass, charging needs and how well it holds charge.
Self-discharge is loss of stored charge while no load is connected. Aging is loss of the ability to hold or deliver charge, even after recharging. Both depend on the cell design, temperature and storage conditions, so a chemistry name is not a shelf-life specification.
A capacity rating also depends on discharge current, temperature and the voltage at which the test stops. Use the particular cell's data, not a single capacity assigned to every AA or D cell.
Common primary alkaline cells serve devices such as clocks, remote controls and flashlights. They are widely available and retain charge relatively well in storage. Their useful capacity and terminal voltage fall more under heavy loads and cold conditions.
They are not intended to be recharged. Leakage can damage equipment, especially when cells are exhausted or left in storage. Rechargeable-battery memory effect is not a useful concern for a primary cell.
NiCd and NiMH are rechargeable nickel batteries
NiCd and NiMH are rechargeable nickel batteries
Nickel-cadmium (NiCd) and nickel-metal hydride (NiMH) use alkaline electrolytes, but they should not be confused with primary alkaline cells.
Two rechargeable nickel families.
Family
Uses and strengths
Limits
NiCd
Legacy cordless tools and industrial backup equipment; capable of substantial discharge currents in suitable designs.
Cadmium is toxic and requires appropriate battery recycling. Repeated partial cycling can cause memory-related voltage depression. Self-discharge matters during storage.
NiMH
Rechargeable consumer cells and hybrid-vehicle packs; generally more capacity than comparable NiCd cells and no cadmium.
Conventional cells can self-discharge noticeably; low-self-discharge versions improve charge retention. Voltage depression can occur, but memory concerns are generally less pronounced than with NiCd.
Use a charger designed for the chemistry and cell. Fast charging is appropriate only when the cell and charger support it. Do not deliberately drive a pack to zero volts to prevent memory effect: a weaker cell can be forced into reverse polarity by the others.
Supporting detail: Addendum 94 — Why a remote-control recommendation needs more than a chemistry name.
Lead-acid trades low mass efficiency for useful power and cost
Lead-acid trades low mass efficiency for useful power and cost
Lead-acid batteries appear in engine starting and stationary backup supplies. They can deliver high starting currents and are relatively inexpensive, but they are heavy for the energy stored.
They self-discharge during storage. Prolonged storage while discharged promotes sulfation, which can reduce capacity; this is not the NiCd memory effect. Starting and deep-cycle designs serve different loads. Use the specified charging method: the electrolyte is acidic, lead is toxic, and charging can release gas. Flooded, absorbed-glass-mat and gel designs all exist; modern lead-acid does not always mean gel.
Lithium-ion needs protection; LiPo is not automatically better
Lithium-ion needs protection; LiPo is not automatically better
Lithium-ion batteries power portable electronics, tools and electric vehicles. Their energy per unit mass is generally considerably higher than NiMH, with relatively slow self-discharge and no routine need for full discharge to prevent memory effect. They still lose capacity through calendar aging and cycling.
Protection and charge control must keep voltage, current and temperature within the cell's limits. A bare cell may not contain its own protection circuit. The pack design must provide the required protection; a protection circuit is not a substitute for a compatible charger.
Lithium-ion polymer, often called LiPo, commonly appears as a light pouch cell in portable devices and model aircraft. The packaging allows thin shapes; some designs support high discharge rates. It does not guarantee higher energy density, lower cost or better resistance to physical damage. Pouches need protection against puncture and crushing. Self-discharge and memory behaviour are broadly those of lithium-ion.
Nominal voltage and charging limits depend on the particular chemistry and cell. Do not use a single voltage for every lithium-ion battery, and do not confuse rechargeable lithium-ion with primary lithium-metal cells.
Battery history moves from a pile to portable rechargeable cells
Battery history moves from a pile to portable rechargeable cells
The important sequence is the change in what batteries made possible.
Volta, around 1800: the voltaic pile made a sustained electrochemical source practical to demonstrate.
Gaston Planté, 1850s: lead-acid introduced a rechargeable battery.
Carl Gassner, 1880s: dry-cell development made the electrolyte easier to contain for portable use. “Dry” means immobilized electrolyte, not absence of moisture.
Waldemar Jungner, 1890s: nickel-cadmium added another rechargeable chemistry.
Lewis Urry, 1950s: work on the modern alkaline cell improved portable primary batteries.
Lithium-ion, 1990s: commercialization enabled rechargeable products with high energy per unit mass, building on earlier work by several researchers.
Supporting detail: Addendum 95 — Scope of this short chronology.
Engineering Fundamentals/Electrical Systems
Battery Capacity and Packs
Convert Ah to Wh, use C-rate and current to estimate performance, and predict the effect of series and parallel cells.
Ampere-hours measure charge; watt-hours measure energy; Practice
Ampere-hours measure charge; watt-hours measure energy
A 2 Ah cell and a 2 Ah battery can store very different amounts of energy if their voltages differ. Ah tells you charge. To estimate energy, you also need voltage.
Energy (Wh) ≈ capacity (Ah) × nominal voltage (V) Energy (J) = energy (Wh) × 3600
For an ideal 2.4 Ah, 3.6 V cell: 2.4 × 3.6 = 8.64 Wh, or 8.64 × 3600 = 31,104 J. Convert mAh to Ah by dividing by 1000 before multiplying by voltage.
Supporting detail: Addendum 96 — Why the battery estimate uses an approximate sign.
C-rate sets a current scale; load current sets ideal runtime; Practice
C-rate sets a current scale; load current sets ideal runtime
A discharge rate of 1C means a current numerically equal to the capacity in Ah divided by one hour. The rate has units of h−1. Here C is a rate notation, not the coulomb symbol.
Rated maximum current (A) ≈ maximum discharge C-rate (h⁻¹) × capacity (Ah) Ideal runtime (h) = capacity (Ah) ÷ load current (A)
A 2.4 Ah cell rated for continuous 3C discharge has a rated current estimate of 3 × 2.4 = 7.2 A. At a constant 1.2 A load, ideal runtime is 2.4 ÷ 1.2 = 2 h. At 3C, the ideal duration is one-third of an hour, or 20 minutes.
A C-rate may describe a test rate, a charge rate, a continuous limit or a short pulse limit. Only a specified maximum discharge rating belongs in the maximum-current equation. Actual pack limits may be lower because of wiring, temperature or protection hardware. A constant-power load also changes current as voltage changes.
Series adds voltage; parallel adds charge capacity
Series adds voltage; parallel adds charge capacity
For matched cells, connect cells in series to increase voltage. Put identical series strings in parallel to increase Ah at the same voltage. 3s2p means three cells per series string and two strings in parallel: six cells altogether.
Pack V = series count × cell V Pack Ah = parallel count × cell Ah Pack Wh ≈ pack V × pack Ah
With 3.6 V, 2.4 Ah cells, a 3s2p pack is 10.8 V, 4.8 Ah and 51.84 Wh. At 3C it has an ideal rated-current estimate of 14.4 A. A 1.2 A pack load gives 4 h ideal runtime.
This is an electrical model, not a pack assembly procedure. It assumes matched cells, balanced series operation and equal current sharing between parallel strings. Real packs need appropriate cell matching, interconnections and protection. See Series and Parallel Circuits.
Explore a pack by changing one input at a time; Interactive; Practice
Explore a pack by changing one input at a time
First double the series count: voltage and energy double, but Ah and runtime at the same pack current do not. Reset it, then double the parallel count: Ah, energy, rated current and ideal runtime double. The load current below is measured at the pack terminals.
Predict first: same current or same ideal power?
Before checking the results, predict whether ideal runtime will stay the same or double in each comparison, and explain what must happen to current. Start with 3.6 V, 2.4 Ah cells in a 3s2p pack at 1.2 A, then try two different meanings of “the same load”:
Same pack current: change only the series count from 3 to 6 and leave the load-current input at 1.2 A.
Same ideal nominal pack power: keep 6s2p, calculate I = P ÷ V = 12.96 W ÷ 21.6 V = 0.6 A, then enter 0.6 A in the existing load-current input.
Paper example: 3.6 V, 2.4 Ah cells; 3s2p; continuous discharge rating 3C; load 1.2 A.
With no JavaScript, use these equations to explore other packs. This example remains in the print view.
Check the fixed-current and fixed-power comparison
Same cells and parallel count, with two different load bases
Case
Nominal voltage
Capacity
Nominal energy
Pack current
Nominal load power
Ideal runtime
3s2p starting case
10.8 V
4.8 Ah
51.84 Wh
1.2 A
12.96 W
4 h
6s2p, same current
21.6 V
4.8 Ah
103.68 Wh
1.2 A
25.92 W
4 h
6s2p, same ideal power
21.6 V
4.8 Ah
103.68 Wh
0.6 A
12.96 W
8 h
Check: at the same current, both packs still have 4.8 Ah, so t = Ah ÷ I stays at 4 h while the 6s2p pack supplies twice the nominal power. At the same ideal power, twice the nominal voltage needs half the current, so the ideal runtime becomes 8 h.
The 6s2p case uses twelve cells instead of six and stores twice the nominal energy. The longer fixed-power runtime is not a free benefit.
This comparison assumes matched cells, constant nominal voltage, the stated Ah is available and the entered load is ideal. It does not predict changing discharge voltage, load or converter losses, reserve capacity, aging, cutoff or protection behavior. The model reports when the requested current exceeds the entered rating; a result below that rating is not a safety certification.
Choose solder, flux, and a tip that transfers heat, then prepare a stable bench and a tinned iron.
Solder melts; the parts being joined do not
Solder melts; the parts being joined do not
Soldering joins metal parts with a filler metal that melts below the parts' melting temperatures. It is closer to brazing than welding: the base metals do not melt. Electrical soldering connects wires, printed circuit boards (PCBs), and electronic components.
A good connection must be mechanically secure and conduct electricity. The molten solder must wet both surfaces: spread onto and bond with them, rather than sit on top as a ball. Clean surfaces, flux, and heat at both parts make that possible.
A temperature-controlled station regulates the iron's tip temperature. A basic iron may have no temperature control; a cordless iron changes how it is powered, not how a joint is made. Check the tool's instructions and choose settings suitable for the solder and components.
Tip shape and size matter. A fine point reaches small spaces, but a chisel's broad face often transfers heat more effectively. Use the largest tinned contact face that fits the joint without touching neighboring connections. Interchangeable tips let one iron handle different work; change them according to the tool's instructions.
Supporting detail: Addendum 97 — What the iron's “sweet spot” means.
Match the solder and flux to electrical work; Practice
Match the solder and flux to electrical work
Leaded solder: common tin-lead alloys melt at lower temperatures than common tin-copper or tin-silver-copper lead-free alloys. Leaded solder is still sold, but lead is restricted in many products. Follow the specified alloy for the work.
Lead-free solder: common electrical alloys use tin with copper and/or silver. They may need a different heating process and can solidify with a duller finish. “Lead-free” does not mean “no fumes.”
Diameter: fine solder wire makes it easier to meter a small amount into a small joint. Thick solder feeds more metal for the same length; it is easy to overfill a small pad.
Flux: helps remove surface oxides during heating so solder can wet the metal. Rosin-core solder carries flux inside the wire; additional compatible electronics flux may help. Do not substitute plumbing acid flux.
Read the alloy and flux label, including any residue-cleaning instructions. See Chemicals and Safety Data Sheets for handling information.
Helping hands or a PCB vise hold the parts still while your hands hold the iron and solder. Keep a proper stand or cradle within reach. Use a damp soldering sponge or brass wool for tip cleaning, and have solder wick (copper braid) or a desoldering pump available for removing excess solder.
It gets hot. Really hot. Park the iron in its stand, and allow the work to cool before touching it. Use ventilation or fume extraction that keeps the plume away from your face and other people; most visible fume comes from flux. Wash your hands after handling leaded solder, and do not eat or drink at the bench.
Supporting detail: Addendum 99 — Further reading on flux fume.
Clean, tin, and keep the working face coated
Clean, tin, and keep the working face coated
With the iron at working temperature, briefly clean the tip on brass wool or a damp soldering sponge. Apply fresh solder to coat its working face, then remove the excess on the cleaner. Leave a thin coating; do not wipe it bare and let it sit hot. Re-tin as needed and before storage as directed by the tool manufacturer.
Heat both parts, feed solder into the joint, let it cool without movement, and inspect the bond rather than its shine alone.
Heat both parts, then feed solder into the joint
Heat both parts, then feed solder into the joint
Prepare the iron and bench using Soldering Equipment and Setup. The iron heats the parts; the heated parts melt the solder. Touch the tinned working face to both wires, or to both the pad and the component lead. Feed solder into the joint, away from the iron's contact point when access allows.
Supporting detail: Addendum 101 — A one-second count is a rhythm, not a temperature test.
Work through the joint in this order; Checklist; Practice
Work through the joint in this order
1. Strip and clean. Expose only the conductor needed for the connection without nicking it. Clean the surfaces to be joined.
2. Support the parts. Form the connection and secure it so it cannot move during soldering.
3. Flux if needed. Use flux compatible with the solder and electrical work.
4. Heat BOTH parts. Put the tinned working face of the iron against both parts at the joint.
5. Feed solder into the heated joint. Let it wet both surfaces. Do not melt a blob on the iron and wipe it onto cold parts.
6. Remove the solder, then the iron. Stop feeding once the connection has enough solder and both surfaces are wetted.
7. Hold still while it cools. Let the solder solidify without moving the connection.
8. Inspect. Check wetting, coverage, clearance from adjacent connections, and damage before powering the circuit.
Look for wetting and shape; shine alone is not a verdict; Practice
Look for wetting and shape; shine alone is not a verdict
A good joint flows onto both surfaces. On a typical through-hole pad, look for a smooth transition from pad to lead, often a concave fillet (an inward-curving slope). Tin-lead joints are often shiny. A sound lead-free joint may be dull; dullness alone does not diagnose a cold joint.
Solder balls up or fails to bond to one surface, often because the parts were not heated adequately. A rough or dull appearance can be a clue, but inspect the contact and shape too.
Disturbed
The connection moved while solidifying, leaving a cracked or disrupted joint. Secure it before reworking.
Too much solder
A large mound hides the connection and makes bridges easier to miss. Remove excess so the joint can be inspected.
Too little solder
The intended connection lacks coverage or a continuous bond. Reheat both surfaces and add only what is needed.
Bridge
Solder joins connections that should be electrically separate. Remove it before applying power.
Keep the circuit disconnected. Secure loose parts, clean and re-tin the tip, and use compatible flux if needed. Reheat both surfaces to remake a poorly wetted or disturbed joint. Use wick or a pump to remove excess solder or a bridge; do not pry at a pad while the solder is solid.
Repeated heating can damage components or lift copper pads from the board. If a joint still will not wet, let it cool and get help finding the cause. Inspect again after repair. A continuity check can help find an open connection or an unintended short, but it does not prove mechanical strength.
Form a supported wire splice, insulate it with heat-shrink, or heat a circuit-board pad and lead together for a through-hole connection.
Make the splice mechanically sound before soldering; Practice
Make the splice mechanically sound before soldering
Solder should not be the only thing holding loose wires in position. Form a stable splice, support it during soldering, and provide strain relief so pulling or bending the cable does not load the soldered joint. Follow the wire and assembly requirements; these sketches show splice shapes, not a qualification standard.
Lay-over or lap: stripped ends overlap alongside one another. Support and strain relief are especially important because the overlap does not lock itself together.
Twist or pigtail: stripped ends twist together and leave the connection on the same side. Cover the joined end completely when insulating it.
Western Union: an inline connection with each free end wrapped around the opposite wire. It is a commonly used, strong splice when properly formed; it is not automatically the best choice for every wire or assembly.
Slide suitable heat-shrink tubing onto a wire before joining it, and keep it away from the soldering heat. After soldering, allow the joint to cool and inspect it. Move the tubing over all exposed conductor, overlapping intact insulation at both ends of an inline splice, then shrink it with the appropriate heat source according to its instructions.
Choose tubing whose unshrunk size passes over the splice and whose recovered size fits the wire. Avoid sharp wire ends that could puncture it. Ordinary heat-shrink provides insulation; do not assume it makes a waterproof connection or replaces strain relief.
Supporting detail: Addendum 103 — When pre-tinning helps.
On a PCB, heat the copper pad and component lead together; Practice
On a PCB, heat the copper pad and component lead together
A pad is the exposed copper connection area on a printed circuit board. A component's lead is its metal leg. In through-hole assembly, the lead passes through a hole in the board. Insert the correct component in the correct orientation and support the board and component before heating.
Place the tinned working face against both the pad and lead. Feed solder into the heated connection and let it flow onto both, then remove solder and iron in that order. Hold still while it cools. Inspect the joint and the gaps to neighboring pads.
Where the component's assembly instructions call for trimming, cut the excess lead above the cooled joint without cutting into the solder fillet. Wear the required eye protection and control the clipped end so it does not fly away or remain on the board. Do not shorten connector pins that must still mate with another connector.
Addendum 1. “It’s not the voltage that gets you, it’s the current”
The saying is true. What usually gets taken from it — that the voltage does not matter
— is not. Current is electricity actually moving through you, and it takes very little of
it to do real harm. Volts sitting on a wire nobody is touching do nothing at all.
Two things together decide how much current you get: how hard the electricity is being pushed,
which is what voltage measures, and how hard your body holds it back, which is called resistance.
Harder push, more current. More resistance, less.
Your resistance is not a fixed number — wet skin holds current back far less than dry
skin does, so the same push moves much more current through you. That half of it cannot be relied
on, which is why the line is drawn on the half that can be: the push.
Addendum 2. The international standards are not one number
On datasheets you will meet a different set of figures, and there the AC and DC limits
are not the same:
50 V AC / 120 V DC
Extra-Low Voltage under
IEC 61140 and IEC 60364-4-41 — 50 V AC rms, or 120 V
ripple-free DC. “Ripple-free” is a real condition, not a figure of speech:
past roughly 10 % rms ripple the supply is treated as AC and the lower number applies.
30 V AC / 60 V DC
Class ES1 in IEC 62368-1, the
standard behind most benchtop and consumer equipment. ES1 is the class that needs no safeguard
at all; ES2 runs up to 50 V AC / 120 V DC and requires one.
Addendum 3. All sixteen sections, and the four OSHA does not enforce
This is OSHA's own list, from Appendix D to 29 CFR 1910.1200. The numbers
and headings are fixed; a manufacturer cannot renumber them or reorder them.
Section 1
Identification — product identifier, recommended use and
restrictions on use, who made it, emergency phone number.
Section 2
Hazard(s) identification — classification, signal word,
hazard statement(s), symbol(s) and precautionary statement(s).
Section 3
Composition / information on ingredients — chemical name,
CAS number, and for a mixture, the ingredients classified as health hazards and how much of
each.
Section 4
First-aid measures — by route of exposure, plus the symptoms
that matter and when to get medical attention.
Section 5
Fire-fighting measures — suitable and unsuitable
extinguishing media, and what the chemical gives off when it burns.
Section 6
Accidental release measures — the spill response.
Section 7
Handling and storage — "conditions for safe storage,
including any incompatibilities".
Section 8
Exposure controls / personal protection — the OSHA
permissible exposure limit, the ACGIH threshold limit value, engineering controls, PPE.
Section 9
Physical and chemical properties — physical state, odor,
flash point, auto-ignition temperature, density, pH and the rest.
Section 10
Stability and reactivity — reactivity, conditions to avoid,
"incompatible materials", hazardous decomposition products.
Section 11
Toxicological information — the health effects and the data
behind them, including any carcinogen listings.
Section 12
Ecological information
Section 13
Disposal considerations
Section 14
Transport information
Section 15
Regulatory information
Section 16
Other information — "the date of preparation of the SDS
or the last change to it".
Twelve through fifteen are the odd ones out.
The headings have to be there: a note to the standard says an SDS "must also include the
headings" for those four, "in order", to stay consistent with the international
system the format comes from. What goes under them is a different question. Appendix D
says "Sections 12-15 may be included in the SDS, but are not mandatory", and a second
note to the same paragraph says "OSHA will not be enforcing information requirements in
sections 12 through 15, as these areas are not under its jurisdiction."
Those four cover the environment, waste, shipping and other agencies' regulations —
EPA and DOT ground, not OSHA's. So Section 13 tells you what the manufacturer suggests doing
with the leftovers. It does not tell you what happens to them here. Ask.
Two more things about the shape of the document. The section order is fixed
but the order within a section is not — preparers "are not required to
present the information in any particular order within each section", so two sheets can
look different inside the same numbered box. And a heading with nothing under it is not an
oversight: where there is no relevant information, "the SDS shall clearly indicate that no
applicable information is available." Read that as nobody has the data — not as
nothing to worry about.
Addendum 4. Signal words, pictograms and H-numbers — how Section 2 is written
There are exactly two signal words, and OSHA defines them in
1910.1200(c): a signal word indicates "the relative level of severity of
hazard", and "'Danger' is used for the more severe hazards, while 'warning' is used
for the less severe."
Severity is relative to the same kind of hazard, and that is the part that catches
people. Flammable liquids in OSHA's Appendix C are the clean example — all three
categories carry the same Flame pictogram, and the signal word is the only
thing separating them:
Category 1
Danger — "Extremely flammable liquid and vapor"
Category 2
Danger — "Highly flammable liquid and vapor"
Category 3
Warning — "Flammable liquid and vapor"
So “warning” does not mean mild. A Category 3
flammable liquid still catches fire. The signal word ranks a hazard against others of its own
kind; it is not a statement that the chemical is safe.
The pictograms are a fixed set of eight — a black symbol in a
red-bordered diamond standing on a point. OSHA names them: Flame, Flame Over Circle,
Exclamation Mark, Exploding Bomb, Corrosion, Gas Cylinder, Health Hazard, and Skull and
Crossbones.
The eight OSHA Hazard Communication pictograms
Flame
Flame Over Circle
Exclamation Mark
Exploding Bomb
Corrosion
Gas Cylinder
Health Hazard
Skull and Crossbones
The H-numbers are an index, not the warning. Real sheets often print a code
such as H225 beside a hazard statement. Those codes come from the international GHS
scheme this format is built on, which treats them as reference labels rather than as a
substitute for the statement itself. OSHA's Appendix C does not use them at all — it
specifies the sentence. Read the sentence.
Addendum 5. Telling a current sheet from an old one
Section 16 carries "the date of preparation of the SDS or the last
change to it." That is the only date on the document, and it is how you tell a live sheet
from one that has sat in a binder for a decade.
Keeping it current is the manufacturer's job, not yours. Under
1910.1200(g)(5), when a manufacturer or importer "becomes newly aware of
any significant information regarding the hazards of a chemical, or ways to protect against the
hazards, this new information shall be added to the safety data sheet within three
months."
Addendum 6. What makes a flammables cabinet “approved”, and how to spot one
OSHA calls it a storage cabinet and defines it by a fire test rather than by
how solid it looks. 29 CFR 1910.106(d)(3) requires cabinets to "limit the
internal temperature to not more than 325 °F. when subjected to a 10-minute fire test",
with all joints and seams staying tight and the door staying closed throughout.
The same paragraph requires the marking, which is the fastest way to recognise one:
"Cabinets shall be labeled in conspicuous lettering, 'Flammable - Keep Fire Away.'"
Addendum 7. The word for this, and where it comes from
“Nip point” is not shop slang. It is the term the machine-guarding standard uses.
29 CFR 1910.212(a)(1) requires guarding against “hazards such as
those created by point of operation, ingoing nip points, rotating parts, flying chips and
sparks.”
OSHA’s Machine Guarding eTool puts it plainly: “In-running nip point
hazards are caused by the rotating parts on machinery.” Its longer treatment,
Concepts and Techniques of Machine Safeguarding (OSHA 3067), gives three kinds:
“Parts can rotate in opposite directions while their axes are parallel to each other.
These parts may be in contact (producing a nip point) or in close proximity.” —
meshing gears.
“Nip points are also created between rotating and tangentially moving parts. Some
examples would be: the point of contact between a power transmission belt and its pulley, a
chain and a sprocket, and a rack and pinion.”
“Nip points can occur between rotating and fixed parts which create a shearing,
crushing, or abrading action.”
So belts, chains, sprockets and gears are rotating hazards by name. What makes them
dangerous is that they draw material in — not that two parts close on each other.
OSHA is just as direct about the plain shaft: “Rotating motion can be dangerous; even
smooth, slowly rotating shafts can grip hair and clothing, and through minor contact force the
hand and arm into a dangerous position.”
These parts are meant to be behind covers, and the standard is specific about it —
29 CFR 1910.219(f)(3): “All sprocket wheels and chains shall be
enclosed unless they are more than seven (7) feet above the floor or platform.”
Addendum 8. What the investigations actually describe
Oregon’s state fatality-investigation program, summarizing the record for this class of
machine: “The most common causes of death and injury from metal lathes include
entanglement of clothing in moving parts, being hit by loose objects on the lathe (e.g.,
chuck keys, tools, metal shavings) and being struck by a part that has not been adequately
secured.” (OR-FACE 2012-18-1, Experienced Journeyman Machinist Killed While
Operating an Engine Lathe, 2014.)
Four investigated deaths, all the same event — something attached to a person touched
something turning, and the machine did the rest:
Smoothing a part while it turned. A 69-year-old machinist with over 30
years’ experience “reached over the work piece to smooth out a radiused transition
with emery cloth and a file in hand” and “his loose clothing (left arm sleeve)
became entangled around the rotating work piece”. A co-worker 30 feet away heard “a
strange ‘winding-up’ sound”. Of that same part, the shop foreman had said that
“the rough surface could grab clothing or gloves”. (OR-FACE 2012-18-1.)
Stock sticking out the back of the spindle. A 52-year-old machinist was
set up on a 103-inch steel bar: “Due to the length of the material, 24 inches were
sticking out the back of the lathe, unguarded, and held in place with a clamping device that
rotates as the lathe rotates.” He reached across the running machine and “the sleeve
of his shirt became entangled”. (Kentucky FACE 21KY002, 2021.)
A burr on the end of the bar. A lathe operator in his twenties had a
1 7/8-inch stub of 1-inch bar standing past the tailstock. “The right pocket of his
shirt was caught by the rotating tailstock burr. His shirt wrapped around the stock and
tightened at the decedent’s neck and chest.” The listed contributing factor is
“walking to and/or reaching over unguarded rotating bar stock”. OSHA makes the same
point in general: the danger “increases when projections such as set screws, bolts, nicks,
abrasions, and projecting keys… are exposed on rotating parts.”
(Michigan FACE 14MI034, 2014; OSHA Machine Guarding eTool.)
A drill press. “As Employee #1 reached into the unguarded point
of operation, his shirt sleeve or gloves became entangled in the drill bit. Employee #1 was
pulled toward the machine, entangling Employee #1’s long hair. The drill press
continued to spin, completely pulling Employee #1 into the operating area.” She died
of her injuries. The same report records that the spindle “had speeds that ranged from 45
to 1115 rotations per minute”. (OSHA accident 114097.015, 20 February 2019.)
Why abrasive cloth keeps appearing. The UK Health and Safety Executive
publishes a sheet on this one task: “Every year there are serious accidents involving the
use of emery cloth on metalworking lathes. These accidents result in serious injuries such as
broken bones, dislocations, lacerations, amputations and occasionally death.” The mechanism
it names is the one above: “Accidents occur when hand-held emery cloth is entangled in the
rotating parts of the machine or where the emery cloth is snagged on the rotating component
dragging the operator into the danger zone.” Its own rules are that emery
cloth “should NEVER be applied directly by hand on manual metalworking lathes”, and
that gloves “increase the risk of entanglement and” are “never acceptable near
rotating parts of machinery”. (HSE Engineering Information Sheet No 2, rev 1,
2015 — that is HSE’s guidance; ask what the procedure is in the shop you are
standing in.)
And the drill press is not the exception it looks like. OSHA’s own
drill-press training script lists, among the ways accidents happen, “getting dangling
jewelry, loose clothing, or hair caught in the drill chuck (rotational hazard)”, and states:
“The primary hazards of drill presses are contact at the point of operation and
rotational hazards. An operator can risk serious hand injury when working too
close to the drilling area, wearing gloves, loose clothing, loose hair, or jewelry.”
Addendum 9. Why belts and chains count as rotating, not pinching
OSHA sorts machine hazards by the motion that causes them, and “pinch point” is
the vocabulary it attaches to parts that travel, not to parts that turn. From
Concepts and Techniques of Machine Safeguarding (OSHA 3067):
Reciprocating motion — “Reciprocating motions may be hazardous
because, during the back-and-forth or up-and-down motion, a worker may be struck by or caught
between a moving and a stationary part.”
Transverse motion, which means movement in a straight continuous line
— “Transverse motion (movement in a straight, continuous line) creates a hazard
because a worker may be struck or caught in a pinch or shear point by the
moving part.”
A belt on a pulley is a rotating hazard that draws material in; a table running up against a
column is a moving hazard that closes on it. Both can take a hand, and the vocabulary is worth
keeping straight because the two do not have the same tell. You avoid the first
by giving it nothing to grip. You avoid the second by knowing where the gap is going.
Guarding is not a local preference. 29 CFR 1910.212(a)(1) —
quoted already in Rotating machinery above for its definition of a nip point — is
a guarding requirement first: one or more methods of machine guarding shall be provided to
protect the operator and other employees from hazards including those created by point of
operation, ingoing nip points, rotating parts, flying chips and sparks.
The reason a rule like this is written without exceptions is that the exceptions are exactly
where people get hurt. A guard comes off for a legitimate setup, the setup takes longer than
expected, somebody else walks up to a machine that looks normal and is not. The standard's own
answer to “but this task genuinely needs the guard off” is not a more
careful operator — it is Lockout/Tagout, the next card on this page, which is
a procedure rather than a permission.
29 CFR 1910.147(a)(1)(i): “This standard covers the servicing
and maintenance of machines and equipment in which the unexpected energization or start
up of the machines or equipment, or release of stored energy could cause injury
to employees.”
Two things are worth reading twice. Unexpected is the whole point — the
hazard is not that the machine runs, it is that it runs while someone has a hand inside it. And
stored energy is named alongside energization, because a machine that has been
switched off and unplugged can still contain everything it needs to move once.
“Servicing and maintenance” is much broader than it sounds. The standard defines it
as “constructing, installing, setting up, adjusting, inspecting, modifying, and
maintaining and/or servicing machines or equipment”, and adds: “These
activities include lubrication, cleaning or unjamming of machines or equipment
and making adjustments or tool changes, where the employee may be exposed to the
unexpected energization or startup of the equipment or release of hazardous energy.” Setting
up, clearing a jam and changing a tool are all on that list.
Stored energy gets its own requirement — 1910.147(d)(5)(i):
“Following the application of lockout or tagout devices to energy isolating devices, all
potentially hazardous stored or residual energy shall be relieved, disconnected, restrained, and
otherwise rendered safe.” The lock comes first, and then the energy already in the machine
is dealt with. Both, in that order.
Addendum 12. Why the chuck key rule is worded as a grip and not as a reminder
A key left in a chuck is launched the instant the machine starts. Written as
“remember to remove the key” the rule depends on you remembering at the one
moment you are busy with something else; written as the key never leaves your hand there
is nothing to remember, because a key that is still in the chuck is still in your hand and you
cannot start the machine.
Do not let a spring be the thing that saves you. Some chuck keys are
spring-loaded and eject themselves when you let go — ours are, on the lathe. Not all keys
are, and our Jacobs chuck keys are not. So the habit has to be the same on every
machine, or it is a habit that works until you walk up to a different chuck.
A drill-press chuck key is lighter than a lathe chuck key and carries far less energy. It is
still dangerous: it is in the list of things that become projectiles in Rotating
machinery above, and “less mass” is not the same as “will not hurt you”
when it leaves a spinning chuck at the distance you are standing.
Addendum 13. Why dry sand is on the list, and why it is probably not on yours
Sand does work. The Aluminum Association’s Guidelines for Handling Aluminum
Fines (F-1) lists fine dry sand, “preferably finer than 20 mesh,” next to
approved dry powders as effective for isolating an aluminum fines fire. It also says
what has to be true first.
Dry. F-1 says dry sand. Damp sand is water, and water
“will react with the aluminum fines to form flammable hydrogen gas.”
Already in the room. “A plentiful supply should be easily available
in the operating area and stored in covered bins or drums.” Sand fetched after the fire
starts is not that.
With the right tool waiting beside it. “Long handled shovels should
be available at each bin or drum, and should be constructed of non-sparking metal.”
Laid, not thrown. The shovels “lay the sand or powder around the
edge or perimeter of the fire.” You are walling it in. Anything thrown at the pile
raises the dust cloud that is the actual explosion.
Decided before it started, by someone senior. “Qualified
supervisory personnel should decide in advance whether it is better to attempt to fight the
fire or to withdraw to a safe location and allow it to burn itself out.”
Those are preconditions, not tips. If you cannot point at the covered sand bin and
the non-sparking shovel beside it right now, you do not have this option — and
the call to fight it was never yours to make on the spot. Alarm, evacuate, report.
Addendum 14. Why technical writing cares about the space
Leave a space between a numerical value and its unit symbol: 8 m,
15.0 kg, and 0.50 s. SI also uses a space before
°C and %. Consistent notation is a
low-cost way to keep a drawing, a spreadsheet, and a controller reading the same thing.
The BIPM SI prefix
table is the primary list used here, including the 2022 ronna, quetta, ronto, and quecto
additions. The NIST SI Units
reference explains SI base and derived units and their technical-writing role.
Addendum 16. Dimensional analysis is also a design check
If a mass density is in kg/m3 and a CAD model volume is in
m3, the cubic meters cancel and the result is kilograms. That is why
CAD mass-property settings, material cards, and drawing units must be read together rather
than as separate menus.
Addendum 17. Two more conversion cases from the unit
Machine run time: an automated machine has operated for 15 years and
150 days. With the stated classroom assumption of 365 days per year,
(15 × 365 + 150) d × (24 h / 1 d) = 135,000 h. Real maintenance
records should use actual calendar dates and include leap days.
Supply-chain fuel: a truck rated 15 mpg has
15 mi/U.S. gal × (1.609344 km / 1 mi) ×
(1 U.S. gal / 3.785411784 L) = 6.37716 km/L. A 150 km one-way route is a 300 km
round trip, requiring 300 km / 6.37716 km/L = 47.0429 L, or
47.0 L, assuming the quoted fuel economy holds for the trip.
The NIST SI Units reference
documents SI base and derived units. The NIST conversion conventions define the inch as exactly
0.0254 m; this page derives square and cubic factors from that exact value. U.S. liquid gallon
values are explicitly labeled whenever they are used.
Addendum 19. The calculus idea, after the practical one
Over a smaller and smaller time interval, average velocity approaches instantaneous
velocity. In calculus notation, velocity is the derivative of position with respect to time:
v = dx/dt. For this course, begin by naming the interval, position change, and
direction correctly; the derivative notation is a compact extension of the same idea.
The NIST SI Units reference
lists velocity as a derived unit example. Direction is an added physical requirement: two
motions may have the same speed but different velocities because their directions differ.
NASA’s
Newton’s second-law resource connects force, mass, and acceleration for grades 9–12.
The calculation here uses the average velocity-change form first; a real machine profile may
have changing instantaneous acceleration within the same interval.
Addendum 22. Check the CAD assumptions before trusting mass properties
Confirm the assigned material, density, document unit, bodies included, and whether the
model represents solid material or an internal void. A precise calculation based on the wrong
material card is still wrong.
NASA Glenn’s
weight-and-mass explanation distinguishes F = ma from
W = mg. The NIST SI
Units reference lists kilograms as an SI base unit and newtons as a derived unit. Those
conventions are used here with g0 = 9.80665 m/s2 for the
standard-gravity examples.
The density conversion is from
NIST
SP 811, Appendix B, which lists slug per cubic foot to kilogram per cubic meter as
5.153 788 E+02; 0.00194032 is its reciprocal.
Engineering Fundamentals/Motion and Rotation/Angular Motion
Addendum 24. Why a radian is barely a unit at all
A radian is an arc length divided by a radius — a length over a length. The two cancel,
so NIST gives the base-unit expression for the radian as m/m and its value as
simply 1: the radian and steradian are “special names for the number one that
may be used to convey information about the quantity concerned.”
That is not trivia. It is why a torque in N·m multiplied by an angle in
rad comes out as energy in joules with no conversion factor anywhere, and why a
formula that mixes rotation with straight-line motion works only when the angle is in radians.
Degrees and revolutions are counts somebody picked; the radian is the ratio the geometry
already contains.
Engineering Fundamentals/Motion and Rotation/Angular Motion
Addendum 25. Where 0.1047198 comes from
One revolution is 2π radians and one minute is 60 seconds, so one revolution
per minute is 2π/60 = 0.104719755… radians per second. It is not a
measured constant; it falls straight out of the two definitions. Turning it over gives
60/(2π) = 9.5492966… revolutions per minute in one radian per second.
Engineering Fundamentals/Motion and Rotation/Angular Motion
Addendum 26. Where these values were checked
NIST
SP 811, Appendix B gives revolution per minute to radian per second as
1.047 198 E−01, revolution to radian as 6.283 185 E+00, and
degree to radian as 1.745 329 E−02. The 9.549297 r/min in one rad/s is the
reciprocal of the first of those.
NIST
SP 811, Chapter 4, Table 3, lists the radian with symbol rad, value
1, and base-unit expression m/m. The rule that every unit symbol takes
a space except the degree, minute, and second of plane angle is
NIST
SP 811, section 7.2.
Addendum 27. Why the radian is the only angle unit that works
A radian is defined as arc length divided by radius. Multiply an angle in radians by a radius
and you get the arc length back — which is exactly the distance the rim travelled. Do the
same thing per second and you have the rim speed. Degrees and revolutions carry an extra
arbitrary count inside them, so they need a conversion factor first. The radian does not,
because it was built out of the same geometry the formula describes.
Conversion factors from
NIST
SP 811, Appendix B: revolution per minute to radian per second 1.047 198
E−01, inch to meter 2.54 E−02 (exact), and mile per hour to
meter per second 4.4704 E−01 (exact).
The grinding-wheel requirement is quoted from
29 CFR
1910.215(d)(1): “The spindle speed of the machine shall be checked before mounting of
the wheel to be certain that it does not exceed the maximum operating speed marked on the
wheel.”
NIST
SP 811, Appendix B lists pound-force foot (lbf·ft) to newton
meter as 1.355 818 E+00, and separately lists foot pound-force
(ft·lbf) to joule as the same 1.355 818 E+00 — the two
entries that establish the word-order convention used above. The reciprocal, 0.7375621, gives
newton metres to pound-force feet.
That M is the prefix symbol for 106 and m the symbol for
the metre is from the prefix and base-unit tables in
NIST
SP 811, Chapter 4.
Engineering Fundamentals/Motion and Rotation/Gear Ratios
Addendum 30. Why tooth counts work, and what the dashed circles mean
The gears here share one tooth size, called module, and a 20° pressure angle. Their pitch diameters are proportional to tooth count. The dashed pitch circles roll together at equal tangential speed, so nA × NA = −nB × NB when clockwise is positive on both shafts. Here n is signed rotational speed and N is tooth count.
Tooth flanks are involute curves. Actual tooth surfaces can slide during contact even though the pitch circles roll. The drawing samples those curves, simplifies the tooth roots and adds a small visual clearance. It is a motion model, not a manufacturing drawing.
The lab assumes rigid external spur gears, fixed shaft centers, matched tooth size and steady transmitted load. It starts lossless; its efficiency control applies the same specified loss to every actual mesh, including both meshes around an idler. Acceleration, elasticity, backlash dynamics, detailed friction, noise and tooth strength are omitted. Changing tooth counts moves the centers to maintain the correct mesh; it does not represent swapping a gear into a fixed gearbox housing.
Engineering Fundamentals/Motion and Rotation/Gear Ratios
Addendum 32. Why adding losses is only an approximation
For a 1000 W input and three 96% stages, the losses are 40 W, 38.4 W and 36.864 W. Each 4% applies to a smaller incoming power. Adding 4% + 4% + 4% incorrectly takes every loss from the original 1000 W.
Engineering Fundamentals/Motion and Rotation/Gear Ratios
Addendum 33. Follow both stages of one loaded train
A 24-tooth driver at 1440 rpm and 4 lbf·ft drives 48 teeth. That shaft also carries a 15-tooth driver for a 45-tooth output. Both stages are 96% efficient, with no other losses. After stage 1: 720 rpm and 4 × 2 × 0.96 = 7.68 lbf·ft. The shared shaft carries that same 720 rpm into stage 2. Final output: 1440/(2 × 3) = 240 rpm and 7.68 × 3 × 0.96 = 22.1184 lbf·ft, versus 24 lbf·ft ideally. Overall efficiency is 0.9216.
Engineering Fundamentals/Motion and Rotation/Gear Ratios
Addendum 34. Worked design: a winch with a speed ceiling and torque floor
A motor supplies 1680 rpm and 24 lbf·ft. The output must be at most 40 rpm and at least 950 lbf·ft. Available gears have 10–60 teeth, with unlimited copies; each reduction stage is at most 6:1 and 97% efficient. There are no idlers or other losses.
Speed requires i ≥ 1680/40 = 42. Two stages give at most 6² = 36, so try three.
Three stages give ηtotal = 0.97³ = 0.912673. Torque requires i ≥ 950/(24 × 0.912673) ≈ 43.3708. Torque controls.
Choose 12 → 48, 15 → 45, and 16 → 60 teeth: i = 4 × 3 × 3.75 = 45. Every tooth count and stage ratio meets its limit.
ωout = 1680/45 ≈ 37.33 rpm ≤ 40 rpm. τout = 24 × 45 × 0.912673 = 985.68684 lbf·ft ≥ 950 lbf·ft. Both pass. Three external meshes make the output opposite to the input.
This is one feasible train, not a claim of an optimum or a complete winch specification. For load force at a drum, continue to Torque; for travel speed, use Rotation and Linear Speed.
Addendum 35. Turning a torque into work, and where the radian goes
A constant torque about a fixed axis that turns through an angle does work: W = τθ, with the angle
in radians. Because the radian is a ratio of two lengths, NIST gives its base-unit expression as
m/m and its value as 1. Nothing is added to the units, so:
1 J = 1 N·m (torque) × 1 rad ·
1 ft·lbf = 1 lbf·ft (torque) × 1 rad
This is the practical payoff of the radian being dimensionless: a motor rated in
N·m turning through an angle in rad gives you joules directly,
with no factor to look up. Use degrees or revolutions instead and the relationship breaks,
because both of those carry a chosen count inside them.
All conversions from
NIST
SP 811, Appendix B: foot pound-force to joule 1.355 818 E+00; watt hour to
joule 3.6 E+03 (exact); kilowatt hour to joule 3.6 E+06 (exact);
British thermal unitIT to joule 1.055 056 E+03, with
Btuth1.054 350 E+03, Btu (mean) 1.055 87 E+03,
Btu (39 °F) 1.059 67 E+03, Btu (59 °F) 1.054 80
E+03 and Btu (60 °F) 1.054 68 E+03 listed separately;
calorieIT to joule 4.1868 E+00 (exact).
The horsepower hour figure is derived rather than quoted: one horsepower is
7.456 999 E+02 watts in the same table, and an hour is 3,600 s, so
745.6999 W × 3,600 s = 2,684,520 J to six figures.
NIST
SP 811, Chapter 4, Table 3, gives the joule as J, expressed as
N·m and in base units as m2·kg·s−2,
and the radian as rad, value 1, base-unit expression
m/m.
One horsepower is 550 ft·lbf/s, which is 550 × 12 = 6,600
lbf·in per second. One revolution per minute is 2π/60 rad/s. Putting a
torque τ in lbf·in and a speed N in rpm into
P = τω gives τN(2π/60) lbf·in per second, and
dividing by 6,600 converts that to horsepower:
Every constant in the shortcut is a unit conversion. Nothing about the physics is buried in
it, which is why the same relationship in coherent SI units needs no constant at all.
NIST
SP 811, Appendix B lists horsepower (550 ft·lbf/s) to watt as
7.456 999 E+02 and horsepower (electric) to watt as 7.46 E+02
— two separately defined units, which is why 745.6999 and 746 both appear above. The
0.001341022 hp in one watt is the reciprocal of the first. Foot pound-force to joule is
1.355 818 E+00 in the same table.
NIST
SP 811, Chapter 4, Table 3, gives the watt as W, expressed as J/s
and in base units as
m2·kg·s−3.
Power factor is defined by
Fluke as
“the ratio of working power, measured in kilowatts (kW), to apparent power, measured in
kilovolt amperes (kVA).” The 63,025 constant is derived above from the horsepower
definition and the rpm-to-rad/s conversion, not quoted.
Addendum 39. What the explorer assumes, and where to check a selection
The explorer compares ordinary drives on parallel shafts. “Separated” means a belt or chain span is practical but a single compact gear pair cannot reach. Speed labels are relative to the chosen component's rating, with no universal rpm cutoff. It excludes load sizing, life prediction, efficiency percentages and automatic cost rankings. “Candidate” means worth sizing, not approved for use.
Addendum 41. Manufacturer references for belt geometry and faults
Gates, Preventive Maintenance Manual, “Belt identification,” “Installation,” and “Belt drive problem diagnosis,” supplies the length/profile distinctions and troubleshooting checks. Gates' industrial synchronous-belt guide explains toothed engagement and dry belt contact. Use the exact belt's data for a real selection.
Addendum 42. Derive the inverse and check speed and wrap
Multiply the length approximation by 4C: 4CL = 8C² + 2π(D + d)C + (D − d)². Set B = 4L − 2π(D + d), giving 8C² − BC + (D − d)² = 0. The quadratic formula gives C = [B + √(B² − 32(D − d)²)]/16. Use this larger root and require C > (D + d)/2 so the pitch circles are separated. An impossible length produces no valid layout.
Assuming no slip, n_small / n_large = D/d and v = πd n_small. With d in mm, divide v by 1000 to get m/min; with d in inches, multiply by 0.0254. Speed n is in r/min; N remains the symbol for teeth.
The tangent-span angle is α = asin((D − d)/(2C)); small-pulley wrap is θ = 180° − 2α, with α expressed in degrees. Less wrap means less grip. The drawing uses circular arcs and tangent spans; the length equation approximates that geometry. Its error grows as (D − d)/(2C) grows, so very unequal, closely spaced pulleys need a more exact calculation for final selection.
The checked ASME public listing names B29.1 as Precision Power Transmission Roller Chains, Attachments, and Sprockets, edition 2011 (R2022). See ASME B29.1. The examples above come from public manufacturer tables, not an unread clause of the paid standard.
Addendum 44. ISO scope and the source of the millimeter dimensions
The ISO 606:2015 public abstract describes short-pitch precision roller and bush chains with associated sprockets. Its scope includes dimensional and strength characteristics; a chain number alone is not a load rating. The dimension examples are from Renold Roller Chain tables, “European (BS) Standard — Simplex.” Renold's Chain Standards guide explains series and strand suffixes.
Addendum 46. Where the formulas come from, and what this model leaves out
Geometry. The pin centres sit on a circle of radius R = p / (2 sin(180°/N)). The leaving pin turns at ω, so its horizontal speed is ωR cos θ and its height above the sprocket centre is R cos θ. The pin hands over to the next one when θ reaches ±180°/N, so v runs from ωR cos(180°/N) to ωR. One pitch leaves per tooth, so the average chain speed is N·p·n. Shigley's text derives the same maximum and minimum exit speeds: Budynas and Nisbett, Shigley's Mechanical Engineering Design, 8th ed., section 17-5, Eqs. 17-30 and 17-31.
Two ways to state the same spread. Tsubaki's Complete Guide to Chain, section 2.2.1 (printed page 15), divides by the fastest speed: (Vmax − Vmin) / Vmax = 1 − cos (180°/N). Shigley's Eq. 17-31 divides the same spread by the average speed. For 9 teeth that gives 6.03 % and 6.15 %. The table shows both columns, and the prediction bands accept either.
Design guidance. Shigley's text adds: For smooth operation at moderate and high speeds it is considered good practice to use a driving sprocket with at least 17 teeth. Follow the chain maker's selection procedure for a real drive.
Left out on purpose. This model has one sprocket with rigid links, pins seated exactly on the pitch polygon, and a taut span kept level. In a real drive the span's far end rides on a second sprocket, so the span also tilts. Tsubaki notes that the centre distance relative to the chain pitch, plus manufacturing and alignment errors, changes how much chordal action you get. The model does not include chain stretch, joint clearance, wear, lubrication, vibration or resonance. The tooth form is drawn schematically, not to a standard tooth profile. Pitch follows the pin-to-pin definition in the first card; the governing standard for these chains is ASME B29.1, linked there.
Addendum 47. Check the size definitions with one gear
A spur gear with 30 teeth and 60 mm reference diameter has m = 60/30 = 2 mm. The diameter is 60/25.4 in, so its equivalent diametral pitch is 30/(60/25.4) = 12.7 teeth/in. In general, m = 25.4/Pd. Two gears can have different diameters and tooth counts while sharing the same tooth size.
Addendum 48. Normal and transverse measurements use different planes
The normal plane cuts across a tooth at right angles to its slant; the transverse plane cuts across the gear at right angles to its shaft. Module (tooth size) and pressure angle can be specified in either plane, so compare values measured in the same plane. For this helical pair, match normal module, normal pressure angle and helix-angle magnitude, with opposite helix hands.
Addendum 49. Primary references for the geometry and helical mesh
KHK, Calculation of Gear Dimensions, sections 4.1 and 4.3, distinguishes reference geometry, profile shifts, and normal/transverse helical dimensions. KHK, ABCs of Gearing, B, develops tooth terminology and spur/helical calculations. KHK's helical-gear catalog gives mating-series and bearing-thrust cautions. Use the mating table for the exact product.
Addendum 50. Why the efficiency and strength comparisons need conditions
The IIT Kharagpur lesson Power Screw Drives and Their Efficiency (sections 6.1.1–6.1.2, hosted by IDC) explains square-thread machining cost, trapezoidal sturdiness, and added friction from inclined flanks. Its force model supports a conditional comparison: hold lead angle, contact friction and other losses comparable. It does not establish a universal ranking against V-thread fasteners.
The buttress working flank makes efficient thrust transmission possible in its intended direction; that is a geometry-based explanation, not a promise of the same measured efficiency as square. Reverse travel is possible, but heavy loading on the opposite flank does not retain the same advantages. Compare actual screw-and-nut ratings, not shape alone.
Addendum 51. Where wear and operating limits enter the selection
Thomson: Lead Screws Q&A — Application Considerations describes sliding-contact heat and wear and the relationship between load and speed. Its discussion also distinguishes the generic lead screw from the ACME form. The absence of radial wedging does not remove contact pressure on the working flank.
NBS Circular 479, Unified Screw Thread Standards, tables 4 and 6, prints the designation entries 1/4, 20, UNC-1A and 1/4, 28, UNF-1A. The examples above omit the class suffix to teach size and pitch. This historical public standard verifies those combinations; it is not a source of current production acceptance limits. The current Unified inch thread standard is ASME B1.1-2024.
NAAMS Metric Fastener Standards, archived sheet F–2.1, dated 05/29/15, lists M6 x1.0 under screw size and M6 x 1.0 under nominal thread diameter and pitch. Only that designation is used here. ISO 261 identifies the general-purpose metric M-thread family; its catalog entry is not being used as a dimension table.
IIT Kharagpur: Friction in Screws, opening page, defines right-handed advance using clockwise rotation away from the person turning the screw. This observer convention avoids ambiguous arrows.
Addendum 54. Check the definition, not just the label on a catalog
Thomson: Screw Pitch and Lead defines lead as nut travel per screw revolution and states the pitch-times-starts relationship. A supplier may list lead directly. Do not multiply a value already labelled lead by the number of starts a second time.
Addendum 55. Derive the 2π from equal power, or one revolution of work
Ideally, power in equals power out: Tω = Fv. With n in rpm, ω = 2πn/60 rad/s and v = nL/60. Cancel n/60 at nonzero steady speed to get F = 2πT/L. Equivalently, one revolution puts in work 2πT and moves the load through L, doing work FL.
With losses, Fv = ηTω. The motion ratio stays fixed, so the reduction appears in force. See Power and Efficiency. At zero speed both powers are zero; this derivation does not predict breakaway torque or static holding capacity. Lowering a load that drives the screw requires a different friction analysis.
Modern Machine Shop's column Eliminate Backlash From Machining Centers (Mike Lynch, 2000) defines backlash as “any non-movement that occurs during axis reversals.” This page uses the CourseWiki definition on Screw Threads: clearance that must be taken up after reversing before the load moves. In a real drive, elastic deflection can add lost motion as well; the lab below leaves it out.
Addendum 57. A readout that measures the slide, and when the clearance still matters
The MIT 2.670 milling machine notes (section “Using the Micrometer Dials”) also point out that a digital readout measures the bed position directly, so its reading is not thrown off by backlash. The clearance is still in the drive. A force that pushes the carriage along the screw can move it across the clearance without the handwheel turning; Climb and Conventional Milling explains when a cutting force does that.
Addendum 58. What the model means, and why it is not a prediction for every CNC
The coordinates describe the cutter relative to the workpiece, viewed from above: +X right, +Y up. A moving table travels in the opposite sense. The drive infers position from motor/screw motion, with no compensation or linear-position correction. The first approach seats both axes and calibrates the coordinates at the start, before the plunge. That reference is kept through the cut.
With positive initial seating, each actual coordinate c is updated as c = min(max(c, q), q + B), where q is the motor-inferred coordinate and B the total clearance. Negative seating uses the band [q − B, q]. These are shifted forms of the same play operator as the screw lab above. Each axis holds until a band edge reaches it. If the axes take up clearance at different moments within a command segment, the actual path has an extra bend; the cutter sweep includes it.
Every cut segment removes a disc swept along that actual segment, a capsule with the cutter's 2 mm radius. The area shading compares the actual and zero-backlash histories at the same command step. Span measurements intersect those capsules with the two centre sections. They are not a best-fit diameter, an overall size tolerance or a guarantee of the rest of the contour.
All other effects are idealized away: no runout, deflection, wear, servo lag, cutting-force pull, thermal error or compensation. Friction is assumed to hold a slide inside its clearance. The shapes, clearance settings and viewing speed are illustrative. Restart begins a fresh workpiece; changing a setting recomputes the experiment.
HEIDENHAIN describes direct linear-axis measurement as working “without intervening mechanical elements”. Such feedback changes what the controller can observe; this lab deliberately does not model that correction. Haas's ballbar interpretation guide distinguishes lost motion at reversal from controller-related reversal spikes. Only rigid lost motion is included here.
Addendum 61. Why two locating supports can create unwanted load
A warming shaft wants to lengthen. If a housing prevents that length change, elastic deformation creates axial reactions. These can consume clearance, increase friction and cause heating. Actual force depends on shaft, bearing and housing stiffness, temperatures and initial clearance. A floating seat also has friction; “radial only” describes its intended support duty, not literally zero incidental axial force.
Addendum 62. Position preload versus spring preload
Position preload sets the bearing rings at a fixed relative distance, for example with shims. Compared with that arrangement, a spring allows more axial movement under an added load. The spring can maintain preload as dimensions change, but the shaft position changes more under load.
No manufacturer restriction confining brass shims to a nonrotating ring was verified. Material and mounting instructions must come from the actual assembly documentation.
Addendum 65. Why voltage and resistance are called derived units
Of the four units above, only the ampere is a base unit — one of the seven that the
rest of SI is built from. The others are derived: their definitions are ratios of units
already defined. NIST expresses the volt as W/A and the ohm as V/A,
and traces both back to base units as
m2·kg·s−3·A−1
and
m2·kg·s−3·A−2.
That is why unit cancellation works on electrical problems exactly as it does on mechanical
ones — the electrical units are made of metres, kilograms, seconds, and amperes underneath.
The technique on Dimensional Analysis does not need a separate electrical version.
Addendum 66. The dropped voltage does not disappear
The power lost in the cord is P = I2R = (10 A)2 × 0.1588
Ω = 15.9 W. That power becomes heat in the conductor, spread along its whole
length.
Notice the squared current. Doubling the load to 20 A does not double the loss, it
quadruples it, to about 64 W. This is why the drop that is harmless on a light load becomes a
real problem on a heavy one, and why the length and gauge of a cord matter more the more current
the tool draws. The condition and routing of the cord itself are covered on
Electrical Safety.
NIST
SP 811, Chapter 4, Table 3, gives: volt V, expressed as W/A, base
units m2·kg·s−3·A−1;
ohm Ω, expressed as V/A, base units
m2·kg·s−3·A−2;
coulomb C, base units s·A; watt W, expressed as
J/s; pascal Pa, expressed as N/m2; and farad
F, expressed as C/V.
The ampere is listed as one of the seven SI base units, with symbol A, by both
BIPM and
NIST. The rule that a unit symbol
takes a capital first letter when the unit is named after a person is
NIST
SP 811, Chapter 6.
Engineering Fundamentals/Electrical Systems/AC and DC
Addendum 68. Why use RMS instead of the average voltage?
A symmetrical sine wave averages to zero over a whole cycle, yet it still heats a resistor. RMS is the DC voltage that would produce the same average heating in that resistance. Square the instantaneous voltage, average those squares over a cycle, then take the square root. The square-root-of-two conversion applies to a sine wave; do not apply it to an arbitrary inverter waveform.
Engineering Fundamentals/Electrical Systems/AC and DC
Addendum 69. Why RMS answers the heating question
Analog Devices' RMS explanation
shows why ordinary signed or absolute averages do not predict heating for arbitrary waveforms. Its
power note
distinguishes average power from the RMS value of a power waveform: RMS voltage or current can calculate
meaningful average power in the stated load. This classroom explorer uses a purely resistive fixed load; it
does not model impedance, power factor, temperature, a meter's coupling mode, or an actual circuit.
Engineering Fundamentals/Electrical Systems/AC and DC
Addendum 70. A comparison with the same power and the same line
In an ideal DC or unity-power-factor comparison, transmitting 8,000 W at 400 V requires 20 A. At 4,000 V it requires 2 A. If the complete line resistance is 0.5 Ω, the losses are 200 W and 2 W. Ten times the voltage gives one hundredth the resistive loss. This simplified comparison omits converter losses and voltage regulation; it is not a design for a real transmission line. For AC loads with a phase shift, see Power and Efficiency.
The historical advantage belongs to the equipment available at the time. Modern converters also make high-voltage DC transmission practical.
Addendum 71. Why a long wire can matter even below its current limit
A wire can stay within its temperature limit yet drop too much voltage for its load. Length increases resistance, and both voltage drop and heating follow from that resistance. The worked cord example in Current, Voltage, and Resistance shows the calculation.
Addendum 72. Definitions used to calculate every result
For AWG number n, diameter d = 0.127 × 92(36 − n)/39 mm. Convert d to meters, then A = πd²/4 in m². Using annealed-copper resistivity ρ = 1.724 × 10−8 Ω·m at 20 °C, R = ρL/A. One foot is exactly 0.3048 m.
With one-way run ℓ, L = 2ℓ and Rloop = ρ(2ℓ)/A. Vdrop = IRloop; percent drop = 100Vdrop/Vsource; Vload = Vsource − Vdrop; wire loss P = I²Rloop. A two-wire single-phase resistive approximation uses the same return path, but this model does not include AC effects.
Addendum 73. Why the parallel formula uses reciprocals
Each branch draws the supply voltage divided by its resistance. Add those branch currents, then divide by the common voltage. The result is a sum of 1/R terms. This reciprocal of resistance is called conductance: parallel branches add ways for current to flow.
Addendum 74. Real meters change the circuit a little
An ideal voltmeter draws no current. A real one has high but finite input resistance. An ideal ammeter drops no voltage. A real one has some resistance and a voltage drop, sometimes called burden voltage. The practice problems use ideal meters unless stated otherwise.
Addendum 75. Check the node count terminal by terminal
The four separate conductor groups are B1+ to S1; the other side of S1 to R1; the other side of R1 to D1 anode; and D1 cathode to B1−. Closing an ideal S1 merges the first two groups into one, leaving three nodes. None of the component bodies is an extra node.
Addendum 76. Where the alignment picture needs care
This is a first picture, not a description of every motor's internal timing. A synchronous motor can rotate at the same speed as the stator field while keeping an angular offset that produces torque. An induction rotor runs slower than the field during normal motoring; that relative motion induces rotor current. A stepper can deliberately stop and hold a commanded position.
Addendum 77. Sources for the torque formula and the commutator
OpenStax, University Physics Volume 2, section 11.5, Force and Torque on a Current Loop, derives the torque on a rectangular loop in a uniform field (equations 11.19 to 11.22). It defines the magnetic moment of an N-turn loop as N·I·A along the loop's normal and describes brushes and a commutator reversing the current. HyperPhysics (Georgia State University), Commutator and Brushes on DC Motor, describes a split-ring device called a commutator that reverses the current as the coil passes the plane perpendicular to the field. Its Torque on a Current Loop page gives the same torque in terms of the magnetic moment.
Addendum 78. Why alternating current alone is not the full explanation
A single winding supplied by single-phase AC makes a field that pulses back and forth; that alone does not establish a starting direction. Single-phase induction motors use an additional starting arrangement. The rotating field, rotor current, and relative speed explain rotation more clearly than saying the rotor field simply opposes the stator field.
Addendum 79. Manufacturer basis for the straight line
maxon's Motor Data and Operating Ranges, p. 10, states: Enhancing the load torque leads to a linear reduction of the speed. It identifies no-load speed and stall torque as the endpoints and specifies fixed applied voltage.
Addendum 80. Derive the halfway result from the straight line
Put x = n/n0. Then T = Ts(1 − x), so P = Tsω0x(1 − x). Since x(1 − x) = 1/4 − (x − 1/2)2, the largest value is 1/4 at x = 1/2. Thus peak power = Tsω0/4, at half no-load speed and half stall torque. The two endpoint maxima cannot occur at the same time.
Portescap's Brush DC Motor Basics, p. 1, point 4, places maximum mechanical power at half the stall torque. On the linear curve, this also means half no-load speed, as derived above.
Addendum 82. Manufacturer basis for the efficiency comparison
Portescap's Brush DC Motor Basics, p. 1, point 3, states: The maximum efficiency is obtained at high speed. Its accompanying torque plot places the efficiency peak below the torque of peak power; the descending speed line therefore puts it at higher speed.
The running conversion follows maxon's gear conversion note: motor speed equals reduction multiplied by load speed, while motor torque equals load torque divided by reduction and gear efficiency. The note also requires checking actual gear torque and speed limits. A separate maxon standstill note explains that power efficiency is undefined when both input and output power are zero. This lesson therefore treats stall as a boundary; it does not calculate blocked-state efficiency or a permissible output torque.
The Uno's internal pull-up is approximately 20–50 kΩ, not a fixed 10 kΩ. Arduino's Uno R3 documentation specifies “20-50k ohm.” At nominal 5 V, a closed switch carries about 0.10–0.25 mA through that resistor, using I = V/R. See Current, Voltage, and Resistance.
Addendum 85. Phototransistor circuits can measure light or switch at a threshold
Vishay's Ambient Light Sensors — Circuit and Window Design shows both light-meter circuits and light-switch circuits. The phototransistor current changes with illumination; the surrounding circuit determines whether the output preserves a range or switches between logic states.
Addendum 86. Why an ultrasonic measurement can be digital
The HC-SR04 manufacturer datasheet, hosted by SparkFun describes an Echo pulse whose width represents the range. Digital describes the two voltage states; the information can be carried by their timing. A single digitalRead tells you the current state, not the pulse duration.
Addendum 87. Arduino's resolution and timing figures
The official analogRead reference source gives “5 volts / 1024 units” and “about 100 microseconds (0.0001 s)”. That is roughly 10,000 reads per second on ATmega-based boards using the usual API, not an absolute ADC hardware limit or a guaranteed loop rate. Computation, communication and delays take additional time. The published analogRead reference is the learner's API lookup.
Addendum 88. Why dividing by 1023 answers a different question
There are 1024 codes but only 1023 intervals between code labels 0 and 1023. Multiplying by 5/1023 stretches those endpoints to exactly 0 and 5 V; that is endpoint scaling, not the nominal ADC step. The explorer and practice consistently use 1024. Real converters have transition offsets, noise and reference error; their exact thresholds are not predicted by this classroom bin model. A code cannot recover the original voltage exactly.
ADC conversion floors each individual ideal sample into a bin. Averaging the reconstructed lower edges therefore need not equal converting the analog sample mean. For a 25% raw 0–5 V sequence with one HIGH and three LOW samples, the analog sample mean is 1.25 V; the lower-edge reconstructions average 4.9951171875/4 = 1.248779296875 V. Neither operation recovers information between sample instants.
Addendum 90. Official frequency table and timer limitations
The Uno R3 row of Arduino's analogWrite reference source states “490 Hz (pins 5 and 6: 980 Hz)”. See also the published analogWrite reference. A frequency near 31 kHz requires changing timer configuration; it is not the stock setting. analogWrite sets duty, not frequency. Arduino's Secrets of Arduino PWM explains prescalers and timer modes. Changing timers can also affect other functions and libraries.
Addendum 91. Why more samples can still give the wrong mean
If the sample clock repeatedly lands at the same PWM phase, every point can read HIGH or every point can read LOW even though the full-cycle time mean is 1.25 V. A sample-and-hold output keeps the most recent point value between samples; holding is not averaging. A carefully spaced finite set can match the cycle mean, but a higher rate or larger count alone does not guarantee an unbiased result. This bounded comparison does not claim reconstruction of an unbandlimited switching edge from a Nyquist test.
During each constant input interval, V(t) = Vtarget + (Vstart − Vtarget)e−t/τ. The model solves for a repeating steady state, then draws the charging and discharging curves. It omits startup, output resistance, component tolerances and loading. At 0% or 100%, the settled output is simply 0 V or 5 V.
Relative motion between a magnetic field and conductors induces a voltage. With a closed circuit, current flows and the shaft must supply work against the electrical load. Motor action and generator action reverse the direction of energy conversion; see Electric Motor Principles. Actual machines and controls determine how they can operate in either direction.
Addendum 94. Why a remote-control recommendation needs more than a chemistry name
A low average load makes charge retention important, but it does not by itself select NiCd over NiMH. Compare the actual cells' self-discharge, usable capacity, voltage and charging requirements. A low-self-discharge NiMH cell behaves differently from an older conventional NiMH cell.
This overview uses the historical sequence in the course generation-and-storage notes, with dates rounded to eras. Invention, patent and market introduction are different milestones; the dates are not intended as a priority claim. The development of lithium-ion was a multi-researcher effort, not solely the work of the company that first sold it.
Addendum 96. Why the battery estimate uses an approximate sign
Wh = Ah × V is exact for constant voltage. A real cell's voltage changes during discharge, so nominal voltage gives an energy estimate. Usable charge also changes with load, temperature, age and the cutoff voltage. These calculations assume the stated capacity is available.
Use the broad, clean, solder-coated working face of the tip against both parts. Do not interpret “side of the iron” as the barrel or an uncoated surface. The useful contact area, not the sharpest point or the highest temperature setting, delivers heat into the joint. A tiny point can be hot and still transfer heat poorly.
Heat applied to a cell can damage its seals and internal parts. Lithium cells in particular can fail dangerously if damaged. Use the intended battery holder or connector instead of applying a soldering iron to a battery.
The UK Health and Safety Executive's guidance for solderers describes rosin-based flux fume and recommends extraction and keeping your head out of the plume.
A hot tip oxidizes. Oxide interferes with wetting, while a solder coating protects the working face and helps make thermal contact with the joint. Tinning the tip is the time to feed solder onto the tip. Making a joint is different: feed solder into the heated joint.
See HAKKO's tip-life guidance for the construction of plated tips and the effects of oxidation.
Addendum 101. A one-second count is a rhythm, not a temperature test
“Apply iron, one-second count, apply solder” reminds you to heat before feeding. The actual time depends on the joint, tip, alloy, and component limits. Look for solder flowing onto both surfaces. If it will not flow, stop and check cleanliness, flux, contact, and tool settings rather than holding the iron there indefinitely.
Addendum 102. Why lead-free solder may look different
Kester's soldering FAQ, under lead-free joint appearance, explains that tin-silver-copper joints can have a dull surface without being poor joints. Judge the connection, not shine alone.
Some wires and terminals are pre-tinned: a small amount of solder wets the surface before final assembly. This can help the final joint flow, but too much solder makes a wire end stiff and bulky. Follow the connection's assembly method and still heat both parts when making the final bond.