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Work, Energy and Power NEET Notes: Complete Guide with Formulas & Solved Examples

Work, Energy and Power
for NEET Physics

Master the concepts of work, kinetic & potential energy, work-energy theorem, power, and collisions — essential for solving mechanics problems, explained for NEET aspirants.

Work Kinetic Energy Potential Energy Work-Energy Theorem Power Collisions
📌 What you'll learn: NEET-level problem solving • All essential formulas • Step-by-step numericals • Quick revision hacks

🔍 Detailed concept explanation

💪 1. Work

Work done by a constant force is W = F·d·cosθ, where θ is the angle between force and displacement. Work is a scalar, unit: joule (J). Positive work: force helps motion (θ<90°); negative work: force opposes motion (θ>90°); zero work: force perpendicular (θ=90°).

⚡ 2. Energy

Kinetic Energy (KE) = ½mv², energy due to motion. Potential Energy (PE) is stored energy. Gravitational PE near Earth = mgh. Spring PE = ½kx² (where x is compression/extension).

🔄 3. Work-Energy Theorem

Net work done by all forces on a body equals change in its kinetic energy: Wnet = ΔKE = ½mvf² – ½mvi². This is a powerful alternative to equations of motion.

📊 4. Conservation of Mechanical Energy

If only conservative forces (gravity, spring force) act, total mechanical energy (KE + PE) remains constant. For non-conservative forces (friction), work done equals change in mechanical energy.

🏎️ 5. Power

Rate of doing work. Average power Pavg = W/t. Instantaneous power P = F·v (dot product). Unit: watt (W).

💥 6. Collisions

Elastic collision: KE and momentum conserved. Inelastic collision: only momentum conserved, KE not conserved (some lost as heat/sound). Perfectly inelastic: bodies stick together. Coefficient of restitution e = relative speed after / relative speed before (e=1 elastic, e=0 perfectly inelastic).

📋 Complete formula sheet

Work W = F·s·cosθ
(variable force: W = ∫F·dx)
Kinetic Energy KE = ½mv²
Potential Energy PEgravity = mgh
PEspring = ½kx²
Work-Energy Wnet = ΔKE
Power P = W/t = F·v
Collision 1D elastic v₁' = (m₁–m₂)v₁/(m₁+m₂) + 2m₂v₂/(m₁+m₂) (head-on)
QuantityFormula
Conservation of MEKEᵢ + PEᵢ = KEf + PEf
Perfectly inelastic collisionvcommon = (m₁v₁ + m₂v₂)/(m₁+m₂)
Loss in KE (inelastic)ΔKE = ½ μ vrel² (μ = reduced mass)
Spring potential energyU = ½kx²

✏️ Solved NEET-level examples

Example 1 (Work & KE)

A 10 kg block is pulled 5 m on a horizontal surface by a force of 50 N at 37° to horizontal. If μk = 0.2, find work done by each force and final speed if starts from rest. (g=10, sin37=0.6, cos37=0.8)

1 Work by applied force: Wapp = F·s·cos37 = 50×5×0.8 = 200 J.
2 Normal force N = mg – F sin37 = 100 – 50×0.6 = 70 N. Friction f = μkN = 0.2×70 = 14 N. Work by friction = –f·s = –14×5 = –70 J.
3 Work by gravity & normal = 0. Net work = 200 – 70 = 130 J.
4 By work-energy theorem: 130 = ½×10×v² – 0 ⇒ v = √26 ≈ 5.1 m/s.

Example 2 (Conservation of energy)

A block of mass 2 kg slides down a frictionless incline from height 5 m. Find speed at bottom and if it compresses a spring (k=1000 N/m) at bottom, find maximum compression.

1 From energy conservation: mgh = ½mv² ⇒ v = √(2gh) = √(2×10×5) = 10 m/s.
2 At spring: ½mv² = ½kx² ⇒ x = v√(m/k) = 10×√(2/1000) = 10×√0.002 = 10×0.0447 ≈ 0.447 m.

Example 3 (Collision)

A 2 kg ball moving at 3 m/s collides elastically with a stationary 1 kg ball. Find velocities after collision.

1 For elastic collision, formulas: v₁' = (m₁–m₂)u₁/(m₁+m₂) + 2m₂u₂/(m₁+m₂). Here u₁=3, u₂=0.
2 v₁' = (2–1)×3/(3) + 0 = (1×3)/3 = 1 m/s.
3 v₂' = 2m₁u₁/(m₁+m₂) = (2×2×3)/3 = 12/3 = 4 m/s.

📈 Important graphs & key points

  • Force–displacement : area under F–x graph = work
  • PE–distance for spring : parabola U = ½kx²
  • KE & PE in SHM : interchange, total constant
  • Power–time : area under P–t = work

⭐ Work done by conservative forces is path-independent and equals negative change in potential energy.

⚡ Quick revision box

Work = F·s·cosθ (scalar, can be +, –, 0)
Energy forms – KE = ½mv², PE = mgh (gravity), ½kx² (spring)
Work-energy theorem – net work = ΔKE
Collisions – momentum always conserved; KE conserved only in elastic

⚠️ Common mistakes to avoid

  • Using work formula W = F·s without considering angle θ.
  • Forgetting that work against friction is negative and dissipates energy.
  • Applying conservation of mechanical energy when non-conservative forces are present.
  • In collisions, mixing up velocity signs – use consistent sign convention.
  • Assuming power P = Fv always; only valid when force and velocity are in same direction.

🧠 Exam strategy tips

  • Identify conservative vs non-conservative forces first.
  • Use work-energy theorem to avoid kinematics when forces are variable.
  • In collision problems, draw before/after diagrams with velocity directions.
  • For spring problems, energy conservation is often easier than force methods.
  • Memorize standard results for elastic collisions (they save time).

❓ Frequently asked questions

📌 Is work done by friction always negative?
Usually yes, because friction opposes relative motion. But if friction provides the force for motion (e.g., walking), it can do positive work on the moving object.
📌 When can we use conservation of mechanical energy?
Only when no non-conservative forces (like friction, air resistance) do work, or when their work is zero.
📌 What is the coefficient of restitution?
It's the ratio of relative speed after collision to relative speed before collision. e = 1 for elastic, 0 for perfectly inelastic.
📌 Does power depend on time interval?
Average power does, but instantaneous power (P = dW/dt) is defined at an instant and does not depend on interval.

⚡ Master Work, Energy and Power – the key to solving complex mechanics problems efficiently. Bookmark this page for last‑minute revision.

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