5.1 Energy conservation
Work done
Work done is force × displacement in the direction of the force. If the force is at angle to the displacement, . The unit is the joule. A force at right angles to the motion does no work, for example the centripetal force on an object in a circle.
Conservation of energy
Work done is how energy is transferred by a force.
Efficiency
Efficiency is often given as a percentage, and it can never exceed 100%. The rest of the energy usually ends up as thermal energy in the surroundings.
Power
Power is the rate of doing work, or the work done per unit time:
The unit is the watt (1 W = 1 J/s).
Deriving P = Fv
A constant force moves an object through a displacement in time . Then , and , so:
If the car is accelerating, the driving force is greater than the resistance. Use , then .
5.2 Gravitational potential energy and kinetic energy
Gravitational potential energy
To lift a mass at steady speed through a height , the force needed equals the weight, . The work done is force × distance:
This holds only where the field is uniform, which means small height changes near the Earth's surface. Chapter 13 deals with larger distances.
Kinetic energy
Take a mass accelerated from rest by a force through a distance , reaching speed . The work done is . From with , , so:
Kinetic energy depends on the square of the speed, so doubling the speed makes it four times as large.
Using energy to solve problems
When there is no friction or drag, the loss of gravitational potential energy equals the gain of kinetic energy, so and . The mass cancels.
Practise this chapter
Every past-paper question on these topics, with the mark scheme.

