Work, Energy and Power — Exam Practice
Practice questions in CBSE, NEET, and JEE Main style covering the work-energy theorem, power, and elastic collisions.
1CBSE Board Exam Style
Yes. Centripetal force is always directed toward the centre, exactly perpendicular to the object’s velocity (which is tangential) at every instant. Since W = Fd cosθ and θ = 90° here, cosθ = 0, so the work done is always zero.
F = ma = m(dv/dt). Work done: W = ∫F dx = ∫m(dv/dt)dx = ∫mv dv (using dx/dt = v).
Integrating from initial velocity u to final velocity v: W = m∫uv v dv = ½m(v² − u²) = KEf − KEi.
(a) Power = rate of doing work = dW/dt = d(F·x)/dt = F(dx/dt) = F·v, for constant force F. This directly connects to the work-energy theorem, since the work being done at this rate is exactly what changes the object’s kinetic energy over time.
(b) P = mgh/t = (200 × 10 × 10) / 60 = 20000/60 ≈ 333.3 W.
2NEET Style (Single-Correct MCQ)
KE = ½mv², and p = mv → v = p/m. Substituting: KE = ½m(p/m)² = p²/2m.
Potential energy requires work done to be path-independent (depending only on start/end position) — true only for conservative forces like gravity and spring force, not for friction or drag.
Power = work/time, so its SI unit, the watt, is exactly one joule per second.
Elastic collisions are specifically defined by the conservation of both quantities — the defining feature that distinguishes them from inelastic collisions.
3JEE Main Style
Loss in PE = gain in KE: mgh = ½mv² → v = √(2gh) = √(2×10×5) = √100 = 10 m/s.
Gravity acts vertically; horizontal displacement is perpendicular to it, so W = Fd cos90° = 0.
U = ½kx² = ½ × 100 × (0.2)² = ½ × 100 × 0.04 = 2 J.

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