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Doing is how energy gets transferred from one store to another. Push a box and you transfer energy to its kinetic store; lift it and you fill its gravitational store. This lesson ties together work done, kinetic and potential energy, and the rate at which energy is transferred — — along with how efficiently a machine does it.
What you'll be able to do
is the energy transferred when a force moves its point of application. It equals the force multiplied by the distance moved . The unit is the joule (J): one joule is transferred when a force of one newton moves through one metre.
If the force acts at an angle to the direction of motion, only the component along the motion does work, so . A force at right angles to the motion (like the tension holding a conker in a circle) does no work at all.
Tip — Watch the angle: it is the angle between the force and the direction of motion. When they are parallel (θ = 0), cos θ = 1 and W = Fs.
is the energy an object has because of its motion. Doing work to accelerate a mass from rest transfers energy into its kinetic store, giving .
Because the speed is squared, doubling the speed quadruples the kinetic energy — which is exactly why stopping distances grow so sharply with speed.
Lifting an object against gravity transfers energy to its store. Near the Earth’s surface, where is effectively constant, the change is .
Only the change in matters, not the path taken — carrying a bag up a ramp or straight up a ladder to the same height needs the same gain in gravitational potential energy.
is the rate of transferring energy, or equivalently the rate of doing work, measured in watts (1 W = 1 J s⁻¹). For a force pushing an object along at a steady speed, power can also be written as force × velocity.
compares the useful energy (or power) output with the total input. It is always less than 1 (or 100%) because some energy is dissipated, usually as heat through friction and resistance.
Equation recap
Common mistakes to avoid
Key takeaways
Test yourself
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