Practice

Work and energy

Kinetic and potential energy, work by a force at an angle, the work-energy theorem, and conservation of energy for falls and springs.

The skill

Work is energy transferred by a force over a distance, and only the component of the force parallel to the displacement counts: W=Fdcos⁡θ. To find a speed, add the work done by every force, positive or negative, and set the sum equal to ΔK. When only conservative forces act inside the system, you can track energy stores instead, ΔUg=mgΔy and Us=12k(Δx)2, with total mechanical energy constant. The common slips are forgetting that friction does negative work and counting gravity twice, once as work and again as potential energy.

A worked example

A 5.5 kg box starts from rest. A horizontal 22 N push moves it 6.3 m across a level floor, while kinetic friction exerts a constant 11 N on it.

What is the box's speed at the end of the 6.3 m, in m/s? Give your answer to three significant figures.

Solution

  1. Net work is the sum of the work done by each force: the push does +138.6 J and friction does −69.3 J, for 69.3 J.
  2. ΔK=ΣWi: 1/2 (5.5) v² − 0 = 69.3, so v = √(2 × 69.3 ÷ 5.5) = 5.02 m/s.

Answer: 5.02

Your turn

Lessons behind these problems