Playbook
Work, Energy and Power
The work-energy theorem, power and collisions. Energy conservation usually beats a force analysis.
- Questions in the bank
- 123
- q/paper in 2025–26
- 0.79
- Numeric answer
- 29%
- Notes pages
- 6
Tier: Long tail
When you’ll see it
A speed after a force has acted over a distance, a spring compressed, a collision or an explosion, or a rate of doing work.
How this chapter is tested
Most questions are short: one energy balance or one momentum balance, then a line of arithmetic. The marks go to choosing the right balance.
The work-energy theorem always holds, as long as every force's work is counted with its sign. Momentum survives every collision and explosion. Kinetic energy survives only an elastic collision, and mechanical energy only where no friction or impact takes any away.
This is a long-tail chapter, and it is often set as a numeric-answer question. The bullet-and-pendulum shape is the standard test of the order: momentum through the impact, energy through the swing.
The sub-skills
The distinct skills inside the chapter, in the order to learn them.
Work by constant and variable forces
W = F·s for a constant force; the integral of F dx, or the signed area under an F–x graph, when it varies with position.
Work-energy theorem and K = p²/2m
The total work of all forces is the change in kinetic energy; for one body, p multiplied by n makes K multiplied by n².
Potential energy and mechanical energy
F = −dU/dx; a spring stores ½kx²; where only conservative forces work, kinetic plus potential energy stays constant.
Power
P = F·v at an instant; under constant power the force falls as the speed rises and x grows as t^(3/2).
Impulse, explosions and sticking collisions
Impulse is the change in momentum; momentum is conserved in an explosion, a recoil or a sticking collision, and kinetic energy is not.
Elastic collisions and restitution
Elastic means momentum and kinetic energy both conserved; e compares separation speed with approach speed, and a bounce height goes as e².
Traps to expect
Distractor shapes this chapter reuses. The Traps page covers the ones that cut across chapters.
Energy conserved through an impact
½mu² = (M + m)gh skips the impact. Use momentum for the impact, then energy for the swing.
Spring energy written as kx²
The stored energy is ½kx², and between two stretches it is ½k(x₂² − x₁²), each measured from the natural length.
Height goes with e, not e²
A ball leaving the floor at e times its arrival speed rises to e² times its starting height, and every bounce is travelled twice.
Constant power taken as constant force
Using v = at and x = ½at² gives x ∝ t². Under constant power x ∝ t^(3/2).
Learn it before you drill it
This chapter has full teaching notes — foundations, worked examples, self-checks and a mastery check for each page. Read the notes once, then drill page by page below.
Work, Energy and Power notesDrill every Work, Energy and Power question
123 questions from the bank, across 6 subtopics.
Drill one subtopic at a time
The 6 subtopics, in teaching order.
- Work Done by Constant and Variable ForcesDrill Work Done by Constant and Variable Forces
- Work-Energy Theorem and Kinetic EnergyDrill Work-Energy Theorem and Kinetic Energy
- Potential Energy and Conservation of Mechanical EnergyDrill Potential Energy and Conservation of Mechanical Energy
- PowerDrill Power
- Impulse, Explosions and Perfectly Inelastic CollisionsDrill Impulse, Explosions and Perfectly Inelastic Collisions
- Elastic Collisions and Coefficient of RestitutionDrill Elastic Collisions and Coefficient of Restitution
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