Work-Energy Theorem
Work, Energy and Power • Class 11 Physics • NCERT • CBSE
The Work-Energy Theorem states: The net work done on a body equals the change in its kinetic energy. W_net = ΔKE = ½mv² − ½mu². Work done W = F·d·cosθ where θ is the angle between force and displacement.
Key Formulas
W = F·d·cosθKE = ½mv²W_net = ½mv² − ½mu²PE (gravity) = mghPE (spring) = ½kx²P = W/t = F·v
Frequently Asked Questions
- When is work done zero even if a force is applied?
- Work done is zero (W = Fdcosθ = 0) when: (1) θ = 90° — force perpendicular to displacement (e.g., a coolie carrying a load on his head while walking horizontally — the load's weight is vertical but displacement is horizontal); (2) displacement = 0 — pushing a wall; (3) force = 0.
- What is the difference between elastic and inelastic collisions?
- In an elastic collision, both kinetic energy and linear momentum are conserved (e.g., billiard balls, gas molecules). In an inelastic collision, only momentum is conserved — some kinetic energy is lost as heat/sound/deformation. A perfectly inelastic collision sees maximum KE loss with the objects sticking together after collision.
- What is the relationship between kinetic energy and momentum?
- Momentum p = mv and KE = ½mv². Therefore KE = p²/(2m). This means: (1) if two objects have same momentum, the lighter one has greater KE; (2) if two objects have same KE, the heavier one has greater momentum.
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