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Work, energy and power

Work is energy in transit, and it has a strict definition that ignores effort entirely: only force along the motion counts. Power is how fast the transfer runs, and one rearrangement of it, P = Fv, explains the top speed of everything with an engine.

Builds on Scalars and vectors.

IN THIS TOPIC

  • Calculate work as W = Fs cos θ, and spot the forces that do no work at all or negative work.
  • Take the work from the area under a force-displacement graph when the force varies.
  • Use P = ΔW/Δt, derive P = Fv from W = Fs, and use it, top-speed problems included.
  • Find efficiency as useful output over input, working in powers or in energies.

COMMON MISCONCEPTION

Work means effort.

What counts as work

In physics, work is energy transferred by a force acting through a displacement.

W=FscosθW = Fs\cos\thetaON THE AQA DATA SHEET

θ is the angle between the force and the displacement, and the cos θ is there for a reason. Only the component of the force along the motion transfers any energy at all.

Only the component of the force along the motion does work: W = F s cos thetaθFF cos θ does the workdisplacement s
FIG. 1A sledge pulled at an angle. The horizontal component F cos θ does the work; the vertical component does none at all.

That definition produces results which offend everyday English. Carry a heavy box across a room at constant height and you do no work on the box whatsoever. Your force is vertical, the motion is horizontal, and cos 90° = 0. Your muscles burn energy and you are genuinely tired, but not one joule of it went into the box.

A force with a component opposing the motion does negative work and takes energy back out. Friction and drag both do it, and the warmth you feel after rubbing your hands together is that energy turning up somewhere else.

WORKED EXAMPLE

Work at an angle

A sledge is pulled 12 m across level snow by a rope at 30° to the ground, with a tension of 40 N.

Only the horizontal component does anything, so W=FscosθW = Fs\cos\theta = 40 × 12 × cos 30° = 420 J to two significant figures.

The vertical component of the tension merely lightens the sledge's press on the snow. It moves nothing vertically, so it transfers no energy.

For a force that varies with position, the work done is the area under the force-displacement graphsFarea = work done
FIG. 2When the force varies with position, the work done is the area under the force-displacement graph.

When the force varies with position, a stretching spring being the standard case, no single F exists to multiply. The area under the force-displacement graph is the work done, for any shape of force.

Power

Power is the rate of doing work, which is the same thing as the rate of energy transfer.

P=ΔWΔt=FvP = \frac{\Delta W}{\Delta t} = FvON THE AQA DATA SHEET

It is measured in watts, one joule per second. The second form is one line of algebra from the first, and that line is worth writing out. A constant force F acting along the motion does work W=FsW = Fs over a displacement s, so dividing by the time taken gives P=Wt=Fst=FvP = \frac{W}{t} = \frac{Fs}{t} = Fv, because s/t is the speed. Nothing new has been introduced. The work equation has simply been divided through by the time. Where the force sits at an angle to the motion, the same cos θ appears in the power equation too, giving P = Fv cos θ.

The Fv form is the one exams lean on hardest. At a vehicle's top speed the acceleration is zero, so the driving force exactly equals the total resistive force, and the engine's maximum power is that force times the top speed. Rearranged the other way, it explains why acceleration fades at speed. Hold the power fixed, raise v, and the available F falls.

GUIDED PRACTICE

Power up the stairs

A 65 kg student climbs a 12 m staircase in 30 s. Find their useful output power against gravity.

Show the working

The useful energy is the gain in gravitational potential energy, mgh = 65 × 9.81 × 12 = 7650 J.

P = E/t = 7650/30 = 255 W ≈ 260 W (2 s.f.). A few light bulbs' worth, and about the most a human body sustains for any length of time. Sprint up the same stairs and the power doubles while the energy stays exactly where it was.

Efficiency

No machine turns all its input into the output you wanted. Efficiency is the useful fraction.

efficiency=useful output powerinput power\text{efficiency} = \frac{\text{useful output power}}{\text{input power}}ON THE AQA DATA SHEET

Quote it as a decimal or as a percentage. The identical ratio works with energies in place of powers, so use whichever pair the question gives you.

Efficiency: the fraction of the input power that comes out as the useful kindinput 100%useful 70%wasted 30%
FIG. 3The input power splits: the cyan branch is the useful output, the amber branch the fraction transferred somewhere useless.

Efficiency can never exceed 100%, so any answer above it is a mistake, almost always the fraction inverted. And the “wasted” share is not destroyed; it is transferred somewhere useless, nearly always ending as internal energy in the surroundings.

INDEPENDENT PRACTICE

An electric winch, realistically rated

A winch draws 500 W of electrical power and lifts a 50 kg load through 8.0 m in 20 s. Find its efficiency.

Show the working

The useful output is mgh/t = 50 × 9.81 × 8.0/20 = 196 W.

Efficiency = 196/500 = 0.39, or 39%. The other 61% ends as internal energy in the motor and the gearbox, which is warm and no use for lifting anything.

ASSESSMENT FOCUS

  • The cos θ is not optional. A rope at an angle does W = Fs cos θ, and the perpendicular component does no work at all.
  • P = Fv is the equation for top-speed problems. At maximum speed the driving force equals the total resistive force, so P = Fres × vmax.
  • CIE asks you to derive P = Fv as well as use it, and the derivation is one line: work is W = Fs, power is that divided by time, and s/t is v. Write those three steps rather than asserting the result.
  • Friction and drag do negative work. Asked for the work done against friction, give the magnitude, and keep your sign convention straight everywhere else in the energy audit.
  • For a variable force, resist the urge to average by eye. The work is the area under the force-displacement graph, counted properly, squares and all.

CHECK YOURSELF

A car of mass 1200 kg travels at a constant 30 m s−1 against total resistive forces of 600 N. What power does the engine deliver, and why does the mass not matter?

Show a hint

Constant speed is a statement about the resultant force.

Show the answer

Constant speed means zero acceleration, so the resultant force is zero and the driving force matches the resistive force at 600 N.

P=FvP = Fv = 600 × 30 = 18 kW.

The mass never enters, because nothing accelerates. Mass could only reach this calculation through F = ma, and a = 0. It is a distractor, and a deliberate one.

Only the force along the motion does any work.

WORKBOOK

Printable practice for this topic: original exam-style questions with room to work, and a fully worked answer book. Free to use; please do not redistribute or sell.

19 questions on this topicAnswer them one at a time and mark yourself against the mark scheme.Practise this topic

Or read them with their mark schemes on the work, energy and power questions page.

8 flashcards on this topicDefinitions, off-sheet equations and a spot-the-error card, scheduled by spaced repetition in your browser.Revise with flashcards

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CHECK YOUR PROGRESS

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  • Calculate work as W = Fs cos θ, and spot the forces that do no work at all or negative work.
  • Take the work from the area under a force-displacement graph when the force varies.
  • Use P = ΔW/Δt, derive P = Fv from W = Fs, and use it, top-speed problems included.
  • Find efficiency as useful output over input, working in powers or in energies.

Open the full revision checklist to track your progress across the whole unit.