Work-Energy theorem is the Swiss Army knife of mechanics — use it when Newton's Laws become messy. Expect 3–4 EAPCET questions every year.
Work, kinetic energy, potential energy, conservation — and when to use each.
Work = Force × displacement component in direction of force.
θ is angle between F and displacement. Work is a scalar.
W > 0: force aids motion. W < 0: force opposes motion (friction, braking). W = 0: force ⊥ displacement (normal force, centripetal force).
KE = ½mv². The Work-Energy Theorem is one of the most powerful tools in mechanics:
Net work done on an object = change in its kinetic energy. Use when forces are complex — no need for acceleration.
Gravitational PE: U = mgh (h = height above reference)
Elastic PE (spring): U = ½kx² (k = spring constant, x = compression/extension)
PE is the energy stored by virtue of position or configuration. It depends on the reference level — only changes in PE are physical.
When only conservative forces do work (gravity, spring — NOT friction):
This is the "no-friction" shortcut. Height and velocity trade off smoothly.
Rate of doing work:
Unit: Watt (W) = J/s. 1 HP = 746 W.
When a machine operates at constant power: P = Fv. As speed increases, the force the engine can exert decreases (for fixed P).
Elastic: Both momentum AND KE conserved. e = 1 (coefficient of restitution).
Inelastic: Only momentum conserved. KE lost as heat. e < 1.
Perfectly inelastic: Bodies stick together. Maximum KE loss. e = 0.
Spring compressed by x stores energy U = ½kx². When released, all PE converts to KE:
For two springs in series: 1/k_eff = 1/k₁ + 1/k₂ (softer combined). In parallel: k_eff = k₁ + k₂ (stiffer combined).
All Work-Energy-Power formulas — exam-ready.
5 problems showcasing when Work-Energy beats Newton's Laws.
4 errors from distractor analysis — conceptual and computational.
Work-Energy is a bridge chapter — it connects kinematics to everything ahead.