🟢 Mechanics · Class 9–12 · Boards + AP + Olympiad

Hold a suitcase all day and you have done no work

W = F·d·cosθ · P = W/t · the work–energy theorem

You will be exhausted, and physics will record zero. Work needs a force AND a distance moved along it, and the arithmetic does not care how tired your arm is. Once you accept that, one short equation connects every push you make to every change of speed that follows.

One definition
W = F·d·cosθ
One rate
Power is work per second
One theorem
Net work = ΔKE
Work · F·d·cosθPower · W/t = F·vTheorem · Wnet = ΔKEUnit · joule, watt
What you'll learn

Work, power and where energy comes from

This page covers work as force times distance along it, the angle that so often makes it zero, power as work per second, and the work–energy theorem that ties them to motion. By the end you'll be able to:

  • Compute work with the angle included, and say when it is zero.
  • Recognise negative work — friction and brakes do it constantly.
  • Use W = ΔKE to get a final speed without touching an equation of motion.
  • Tell power from energy — the same climb, taken at two speeds.
  • Drive the Work Bench and watch the area under the graph become the energy bar.
Why it matters · where it's tested

The bridge between force and energy

Everything before this chapter is forces; everything after it is energy. The work–energy theorem is the sentence that joins the two halves of mechanics:

CBSE · Class 9 — Work and Energy CBSE · Class 11 — Work, Energy and Power ICSE — Work, energy and power IGCSE · Cambridge / Edexcel — Energy AP Physics 1 — Work and energy Olympiad — NSO · NSEJS foundations

Searched as: work done formula, w = fd cos theta, work energy theorem, power formula, why is holding not work, negative work.

Formulas at a glance

Depth guide: 🟢 Class 9–11 must-know · 🟡 useful · 🔴 extension
FormulaMeaningUnitLevel
W = F·d·cosθTHE DEFINITION — only the force ALONG the motion counts
θ is the angle between the force and the displacement
joule (J)🟢
Wnet = ΔKETHE THEOREM — net work equals the change in kinetic energyJ🟢
KE = ½mv²The energy an object has by movingJ🟢
P = W/tPower — work done per secondwatt (W)🟢
P = F·vThe same power, for a steady force at a steady speedW🟡
PE = mghWork done against gravity, stored and returnableJ🟢
W = area under F–dFor a changing force, the work is the area on the graphJ🔴

See it live

Predict the final speed, lock it, then drag the block and watch the area under the force graph turn into kinetic energy. 🟢 real work–energy engine

Work Bench

Work by you60 J
Work by friction−20 J
Net work40 J
Final speed4.0 m/s
Predict first: how fast will it be going at the end, in m/s?

Guess, then lock — the bench waits until you commit.

Try one
W = F·d·cosθ → 60 J
→You push
→It moves
→Net work is done
→The speed changes
Set a force and a distance to start.

Set your force, the distance and the angle — then watch what reaches the block as energy.

Is that work?

Before any arithmetic, decide whether any work is being done at all. Six situations — your answers build the table underneath.

Situation 1 of 6
Named: 0 of 6

Holding a suitcase still. What work is being done on it?

Ask two things: is there a force, and has it moved anything along itself?

SituationWorkWhy

The angle between the force and the motion settles every one of these.

Hit the final speed

A 2 kg trolley starts at rest. Choose a force so that after 4 m it is moving at the target speed — 3 attempts.

3 tries
Attempts left: 3

Set the force, then push. W = F·d becomes ½mv².

Impossible work — what is wrong?

Each claim breaks the definition somewhere. Tap the broken idea.

What is impossible?

Work is force multiplied by the distance moved along it. With no movement there is no distance, so the work on the box is zero however long it is held.

What is impossible?

Friction opposes the motion, so the angle between it and the displacement is 180° and cos180° is −1. Its work is negative: it takes energy out.

What is impossible?

Work against gravity is mgh and contains no time at all. Running changes the POWER, which is work per second, not the work itself.

Always · Sometimes · Never

Thinking beats memorising. Sort every claim about work into three boxes.

Always

  • W = F·d·cosθ, with θ between force and displacement
  • Net work equals the change in kinetic energy
  • Power is work divided by the time it took

Sometimes

  • The work is negative (friction, brakes, lowering a load)
  • The work is recoverable (lifting, stretching a spring)
  • A force does no work at all despite being large

Never

  • Work done on something that has not moved
  • Time appearing in the formula for work
  • A force at 90° to the motion doing work

Positive, negative or zero?

One force, one motion, one decision. The sign of work is where most marks are lost.

Read the arrows
Score: 0 of 0
The work done by that force is

Compare the direction of the force with the direction of the movement.

Choose the motor

Pick a lifting job, then choose a motor. The energy is fixed by the load and the height; the motor decides only how long it takes.

Job: 200 kg, 10 m, 20 s
Not yet

Work is mgh. Power is that work divided by the time you are allowed.

Everyday detective

Read the scene. All three are about the difference between work and power.

You walk up the stairs today and run up them tomorrow. What changes?

Same you, same height, so the same mgh of work. Running delivers those joules in fewer seconds, which is more power — and that is precisely what makes it hard.

What is the braking force doing, in energy terms?

The force opposes the motion, so cos180° = −1 and the work is negative. That negative work is exactly the kinetic energy being removed, and the brakes get hot by the same amount.

How much work does gravity do on it over one orbit?

In a circular orbit gravity is at 90° to the velocity at every instant, so cosθ is zero throughout. That is exactly why the satellite's speed never changes and it needs no fuel.

What's going on

In plain terms: work is the way energy gets moved from one place to another by a force. If nothing moves along the force, nothing is transferred.

Only the part along the motion counts

Push at an angle and your force splits into two parts: one along the motion and one across it. Only the first does any work, which is why the formula carries cosθ. At 90° the whole force is across the motion and the work is exactly zero, no matter how large the force is — this is why carrying a bag on the level does no work against gravity.

Negative work is not a trick

A force pointing against the motion has θ = 180°, cosθ = −1, and does negative work. Friction always does. So do brakes, and so does gravity when you lift something. Negative work means energy is being taken OUT of the object's motion — which is precisely what slowing down is.

The theorem that shortens everything

Wnet = ΔKE. Add up the work done by every force, and the total equals the change in ½mv². You never need the acceleration, the time, or even the shape of the path. Messy forces over a messy route still give the final speed in one line, which is why this theorem is worth more than it first appears.

Edge cases worth knowing

A centripetal force does no work at all, because it is always perpendicular to the motion — which is why orbital speed is constant. Power can also be written P = F·v, so the same engine delivers more power the faster you are already going. And for a changing force, the work is the area under the force–distance graph, which is where a spring's ½kx² comes from.

Solve it with me, step by step 🟢 Class 9–12

Exams reward the method. Work it one step at a time — read the thought, predict the line, then reveal it.

See the maths

Three small labs, each one native to this idea.

1 · The angle, and what it costs you

Same force, same distance. Turn it away from the motion and watch the work fall to nothing.
W
60 J
W = F·d·cosθ · F = 20 N · d = 3 m

2 · Work in, speed out

The theorem drawn: joules on one axis, metres per second on the other. Not a straight line.
v
6.0 m/s
v = √(2W/m) · m = 2 kg

3 · Same work, different power

One climb, taken at different speeds. The joules never move; the watts do.
P
470 W
W = mgh = 2352 J · 60 kg up 4 m

The word that had to be narrowed

1826

Coriolis names it

Gaspard-Gustave de Coriolis proposed using "work" for force times distance, to give engineers a single number for what a machine actually delivered.

1829

Machines get a common currency

His book on the calculation of machine action let a water wheel, a horse and a steam engine be compared by the same measure for the first time.

1840s

Joule ties work to heat

James Joule showed that mechanical work and heat are the same currency, which is why the unit of both now carries his name.

1882

The watt is adopted

The unit of power was named for James Watt, whose engines had been sold in horsepower — a marketing figure he invented to compare against the animals he was replacing.

Today

Still two different words

Everyday speech still uses "work" for effort and "power" for importance, which is why this chapter spends most of its time on definitions.

In the real world

A crane on a building site

The energy per lift is mgh whatever motor you fit. The motor's rating decides only how many seconds each lift takes.

Stairs, walked or run

Identical work either way. Running compresses the same joules into fewer seconds, which is the whole of why it is harder.

An engine at speed

P = F·v means the same thrust delivers more power the faster you already are, which is why acceleration eases off near top speed.

From lifting a book to a rocket launch 🟡

Drag the slider. Six jobs, from a few joules to a few hundred gigajoules.

bookstairsliftcranetrainrocket

Climbing stairs

about 2.4 kJ

Eleven orders of magnitude, and the same three letters underneath every one.

Build it yourself — science-fair projects

Each one is a build and a measurement — the measuring is what turns a demo into a project.

🪜Beginner

Measure your own power

Shows · P = mgh/t

Build: a flight of stairs, a tape measure and a stopwatch.

Measure: your mass, the total height, and the time. Compare walking with running — same joules, different watts.

📐Beginner

The angle experiment

Shows · cosθ is real

Build: a trolley pulled the same distance by the same spring balance, at several rope angles.

Measure: the final speed each time. The flatter the rope, the faster it ends up.

🎯Intermediate

Work in, speed out

Shows · W = ½mv²

Build: a trolley pulled by a hanging weight over a known distance, with a timing gate.

Measure: the speed for several distances, then plot v² against distance. It should be a straight line.

🪢Intermediate

The spring's area

Shows · W is the area under F–x

Build: a spring stretched in steps, with the force recorded at each extension.

Measure: plot F against x and find the area under it. Compare with ½kx².

🛒Champion

Where did the energy go?

Shows · negative work by friction

Build: a trolley given a known push, allowed to run until it stops.

Measure: its initial kinetic energy and the distance it travelled; divide to get the friction force, then check it against μmg.

🚢Champion

Pulley advantage

Shows · work is conserved

Build: a load raised directly, then through a two-pulley system.

Measure: force and distance in both cases. The force halves, the rope length doubles, and the work barely changes.

Glossary — the 10 words that unlock it

Work

What it means
Force multiplied by the distance moved along it.
Why it matters
It is how energy is transferred by a force.
Example
20 N over 3 m is 60 J.
Key question
What makes it zero?

Joule

What it means
One newton acting through one metre.
Why it matters
It is the unit of work, energy and heat alike.
Example
Lifting a small apple one metre.
Key question
Why is heat measured in the same unit?

Power

What it means
Work done per second.
Why it matters
It is the rate, not the total.
Example
2352 J in 5 s is 470 W.
Key question
Can two jobs have equal work and unequal power?

Kinetic energy

What it means
½mv² — the energy of moving.
Why it matters
Net work changes exactly this.
Example
2 kg at 6 m/s carries 36 J.
Key question
What happens if the speed doubles?

Potential energy

What it means
mgh — work stored by lifting, returnable later.
Why it matters
Gravity gives it back on the way down.
Example
A 1 kg book on a 2 m shelf holds about 20 J.
Key question
Does the route up matter?

Work–energy theorem

What it means
Net work equals the change in kinetic energy.
Why it matters
It gives a final speed with no acceleration and no time.
Example
36 J into 2 kg at rest gives 6 m/s.
Key question
Does the shape of the path matter?

The angle θ

What it means
The angle between the force and the displacement.
Why it matters
cosθ decides how much of the force counts.
Example
At 90° the work is exactly zero.
Key question
Which two directions is it between?

Negative work

What it means
Work by a force opposing the motion.
Why it matters
It takes kinetic energy out.
Example
Friction, brakes, gravity on the way up.
Key question
Where does that energy end up?

Watt

What it means
One joule per second.
Why it matters
Every motor and appliance is rated in it.
Example
A fit adult sustains a few hundred.
Key question
Is a watt an amount or a rate?

Horsepower

What it means
About 746 W — a unit Watt invented for selling engines.
Why it matters
It is a marketing measure that outlived its purpose.
Example
A 100 hp car is about 75 kW.
Key question
Could a horse sustain one?
हिन्दी · key words Work · कार्य Energy · ऊर्जा Power · शक्ति Force · बल Distance · दूरी

The questions people ask

Straight answers, each one complete on its own:

Why is holding something heavy not work?
Why

Work is force multiplied by the distance moved along that force. A held object does not move, so there is no distance and the work done on it is zero. Your muscles do burn energy, because they hold tension by contracting and relaxing constantly, but that energy goes into your body rather than into the object.

What does the cosθ actually do?
What

It picks out the part of the force that lies along the motion, because only that part transfers energy. At 0° the whole force counts, at 60° half of it does, and at 90° none of it does. The angle is measured between the force and the displacement, not between the force and the ground.

How can work be negative?
How

When the force opposes the motion, the angle is 180° and cosθ is −1. Friction, brakes and gravity on an object moving upwards all do negative work, which means they are removing energy from the object's motion rather than adding to it. That removed energy has to go somewhere, usually as heat.

What is the work–energy theorem for?
How

It says the total work done by all the forces equals the change in kinetic energy. That lets you find a final speed without knowing the acceleration, the time, or even the shape of the path — which is often far quicker than using F = ma and an equation of motion, and sometimes the only practical route.

What is the difference between work and power?
Comparative

Work is the total energy transferred, measured in joules. Power is how fast it is transferred, measured in watts, which are joules per second. Climbing the same stairs slowly or quickly involves the same work; only the power differs, and it is the power that makes the fast climb feel hard.

Does a centripetal force do work?
Scenario

No. It is always perpendicular to the motion, so cosθ is zero at every instant and the work is zero over any path. This is exactly why an object in uniform circular motion keeps a constant speed, and why a satellite in a circular orbit needs no fuel to stay there.

Why is work measured in the same unit as heat?
Why

Because they are the same quantity in different forms. Joule's experiments showed that a fixed amount of mechanical work always produced the same amount of heat, which established energy as a single currency. That is why the joule is used for work, kinetic energy, potential energy and heat alike.

What if the force keeps changing?
How

Then the work is the area under the force–distance graph rather than a simple product. For a constant force that area is a rectangle, F × d. For a spring, where the force grows as you stretch it, the area is a triangle and gives ½kx², which is exactly the elastic energy stored.

Common mistakes — and the fix 🟢 Class 9–12

Spot these before the exam does.

The slipThe fix
Leaving cosθ out of the formulaOnly the component along the motion counts
Measuring θ from the groundθ is between the force and the displacement
Writing friction's work as positiveIt opposes the motion, so it is negative
Putting time into the work formulaTime belongs to power, not work
Using the applied work in W = ΔKEThe theorem needs the net work
Forgetting the ½ in kinetic energyKE = ½mv², and v is squared

Test yourself — a mixed set

Seven question formats, the way LLOS.ai serves them — multiple choice, multiple-correct, fill-in-the-blank, match, sequence, read-think-connect, and write-your-own. Every question has layered hints: a quick nudge, the reasoning, then a deeper connection — so a wrong answer opens a door, never a dead end. 🟢 received from a board-tagged question bank · seed toward 2,000

Pick your board — the set re-tunes to its wording and emphasis. Competitive draws the JEE / NEET / Olympiad lane.

Loading the question bank…
Question 1 of 16
Multiple choice

Which does the most work?

Four efforts, no numbers yet. Tap them in order, most work first. Then read what W = F·d·cosθ gives — and see what fooled you.

Your ranking
Picked: 0 of 4
A · the exhausting one

Holding a 30 kg crate steady at chest height for a full ten minutes, arms shaking.

B · the sideways one

Carrying that same 30 kg crate fifty metres along a flat corridor.

C · the gentle one

Sliding a 10 kg box four metres across a floor with a steady 25 N push.

D · the short one

Lifting the 30 kg crate from the floor onto a bench one metre up.

Tap the four in the order you believe, most work first.

Key takeaways

  • W = F·d·cosθ — only the force along the motion does any work.
  • No movement means no work, however hard the effort feels.
  • Negative work is normal: friction and brakes do nothing else.
  • Wnet = ΔKE gives a final speed with no acceleration and no time.
  • Power is the rate, so the same climb can cost the same joules at very different watts.

Where this lesson leads

This chapter is the hinge between forces and energy, and everything after it uses both:
✓Work and its angle
✓The work–energy theorem
✓Power
→Conservation of energy
→Springs and elastic energy
→Collisions and momentum

Keep exploring

Effort is what you feel. Work is what arrives. The gap between those two words is most of what this page has been about.

Copyright © Pawan Nayar · LLOS.ai · 2026 — Original pedagogy, voice, and design — all rights reserved.
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