Complete Solutions and Summary of Work, Energy and Power – NCERT Class 11, Physics, Chapter 5 – Summary, Questions, Answers, Extra Questions

Summary of work, kinetic and potential energy, work-energy theorem, power, energy conservation, spring energy, and collision with solved NCERT problems.

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Categories: NCERT, Class XI, Physics, Summary, Work, Energy, Power, Work-Energy Theorem, Mechanical Energy, Chapter 5
Tags: Work, Energy, Power, Kinetic Energy, Potential Energy, Work-Energy Theorem, Conservation of Energy, Spring Energy, Collisions, NCERT, Class 11, Physics, Chapter 5, Answers, Extra Questions
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Work, Energy and Power Class 11 NCERT Chapter 5 - Ultimate Study Guide, Notes, Questions, Quiz 2025

Work, Energy and Power

Chapter 5: Physics - Ultimate Study Guide | NCERT Class 11 Notes, Questions, Examples & Quiz 2025

Full Chapter Summary & Detailed Notes - Work, Energy and Power Class 11 NCERT

Overview & Key Concepts

  • Chapter Goal: Define work precisely using vectors (scalar product), introduce kinetic and potential energy, derive work-energy theorem, discuss conservation of mechanical energy, power, and collisions. Exam Focus: Work \( W = \vec{F} \cdot \vec{d} \), KE \( \frac{1}{2}mv^2 \), PE \( mgh \), spring \( \frac{1}{2}kx^2 \), power \( P = \frac{dW}{dt} \). 2025 Updates: Reprint emphasizes variable forces, integrals for work. Fun Fact: Joule’s paddle wheel experiment unified heat/work. Core Idea: Energy conserved in isolated systems; work changes KE. Real-World: Cars (KE to heat via friction), pendulums (PE to KE). Ties: Builds on vectors (Ch.3), leads to gravitation (Ch.7).
  • Wider Scope: Foundation for thermodynamics (Ch.11), rotational dynamics (Ch.7); applications in efficiency, renewable energy.

5.1 Introduction

Everyday terms 'work', 'energy', 'power' differ from physics: Work is force times displacement (scalar product); energy is capacity to do work; power is work rate. Physics definitions precise to quantify changes. Depth: Physiological 'work' (e.g., studying) ≠ physical (no displacement). Historical: Correlates loosely with stamina (energy). Real-Life: Farmer ploughing does work if force displaces soil. Exam Tip: Work zero if no displacement or perpendicular force. Extended: Chapter unifies motion (Ch.4) with energy; prerequisite scalar product for \(\vec{F} \cdot \vec{d}\). Links: Calculus for variable forces (integration). Applications: Engineering (work in machines). Pitfalls: Confuse with colloquial use (e.g., holding weight = no work). Graphs: Force-displacement for work area. Symbols: Bold vectors, J for joule. Coherent SI units.

  • Examples: Lifting book (work against gravity), walking (work if friction).
  • Scalar Product Need: Vectors like force/displacement multiply to scalar work.

Extended Discussion: Energy crisis relevance; chapter focuses conservative forces (path-independent work). Vector language: Dot for projections. Advanced: Relativistic energy \( E = mc^2 + KE \). Real-Life: Solar panels convert light energy to electrical work. Errors: Forget cosθ in work. Tips: Always specify direction.

5.1.1 The Scalar Product

Dot product \(\vec{A} \cdot \vec{B} = AB \cos\theta\): Scalar from two vectors, θ angle between. Properties: Commutative (\(\vec{A} \cdot \vec{B} = \vec{B} \cdot \vec{A}\)), distributive (\(\vec{A} \cdot (\vec{B} + \vec{C}) = \vec{A} \cdot \vec{B} + \vec{A} \cdot \vec{C}\)), \(\vec{A} \cdot (\lambda \vec{B}) = \lambda (\vec{A} \cdot \vec{B})\). Components: \(\vec{A} \cdot \vec{B} = A_x B_x + A_y B_y + A_z B_z\). Magnitude: \(\vec{A} \cdot \vec{A} = A^2\). Perpendicular: Dot=0. Depth: Projection: \( A \cdot (B \cos\theta) \). Real-Life: Work = force projection on displacement. Exam Tip: Unit vectors \(\hat{i} \cdot \hat{i} =1\), \(\hat{i} \cdot \hat{j}=0\). Extended: In 3D, full components. Ties: Ch.3 vectors; used in work, power. Applications: Projections in mechanics. Graphs: Fig.5.1 triangles for cosθ. Symbols: Dot notation. Pitfalls: θ=0 max, 90° zero, 180° negative.

  • Example 5.1: Force (3i+4j-5k), disp (5i+4j+3k); dot=16, cosθ=0.32, θ=71.3°.
  • Proofs: Left as exercise; derive from geometry.

Extended: Vector product (cross) in Ch.6 torque. Advanced: Tensor products. Real-Life: Dot in computing (similarity). Errors: Confuse with cross (vector). Tips: Use components for calc.

5.2 Notions of Work and Kinetic Energy: The Work-Energy Theorem

From kinematics \( v^2 - u^2 = 2as \), multiply m/2: \( \frac{1}{2}mv^2 - \frac{1}{2}mu^2 = Fs \). Vector: \( \Delta K = \vec{F} \cdot \vec{d} \). WE Theorem: Change in KE = net work done. Depth: Motivates definitions; K scalar, work scalar. Real-Life: Braking car (negative work reduces KE). Exam Tip: For constant F; generalizes to variable. Extended: 3D \(\vec{v}^2 - \vec{u}^2 = 2 \vec{a} \cdot \vec{d}\). Ties: Ch.3 motion. Applications: Raindrop Ex5.2: Wg=10J, Wr=-8.75J, ΔK=1.25J. Graphs: Speed-time for KE. Symbols: K for kinetic. Pitfalls: Net force only. Advanced: Relativistic KE approx.

  • Example 5.2: Raindrop m=1g, h=1km, v=50m/s; ΔK=1.25J, Wg=10J, Wr=-8.75J (resistive negative).
  • General: \( K_f - K_i = W \).

Extended Discussion: Theorem integral form of F=ma; loses time info. Real-Life: Sports (work to accelerate ball). Errors: Forget vector dot. Tips: Use for energy changes.

5.3 Work

\( W = \vec{F} \cdot \vec{d} = F d \cos\theta \): Component along displacement times d. Units: J (Nm). Zero if: d=0 (hold weight), F=0 (frictionless), θ=90° (gravity on horizontal). Positive θ<90°, negative >90° (friction). Depth: Dimensions [ML²T⁻²]. Real-Life: Pushing wall (F large, d=0, W=0; tired from internal energy). Exam Tip: Friction always negative work. Extended: Table 5.1 alternative units (eV, cal). Ties: Scalar product. Applications: Cyclist Ex5.3: Wr=-2000J (road on cycle), cycle on road=0 (no d). Graphs: F-d line for W area. Symbols: θ between F and d. Pitfalls: Perpendicular cos0=0.

  • Example 5.3: Cyclist stop 10m, F=200N opp; Wr=-2000J, cycle on road=0 (Newton III, but d=0).
  • Newton III: Forces equal opp, but work not (diff d).

Extended: Path-dependent for non-conservative (friction). Advanced: Virtual work principle. Real-Life: Weightlifter holds=0 work. Errors: Assume always positive. Tips: Specify θ.

5.4 Kinetic Energy

\( K = \frac{1}{2} m v^2 \): Measure of work object can do via motion. Scalar. Depth: From WE theorem. Real-Life: Table 5.2: Bullet 1000J, car 3.5×10⁵J. Exam Tip: Depends v², not direction. Extended: Relativistic \( (\gamma -1)mc^2 \). Ties: Ch.2 speed. Applications: Bullet Ex5.4: Initial 1000J, final 100J, vf=63.2m/s (68% reduction). Graphs: v-t for K. Symbols: J. Pitfalls: Zero at rest. Advanced: Molecular KE= (3/2)kT. Real-Life: Windmills harness KE. Errors: Confuse with momentum (mv). Tips: Half mv².

  • Example 5.4: Bullet 50g, 200m/s plywood 2cm; 10% KE out, vf=63.2m/s.
  • Intuitive: Fast stream grinds corn.

Extended Discussion: KE theorem for particles. Real-Life: Athletics (running KE). Errors: Units kg m²/s². Tips: Calc ΔK.

5.5 Work Done by a Variable Force

For F(x) varying: Approximate rectangles ΔW=FΔx, sum to integral \( W = \int_{x_i}^{x_f} F(x) dx \) (area under curve). Depth: Limit Δx→0. Real-Life: Woman pushing trunk Ex5.5: WF=1750J (rect+trapezium), Wf=-1000J. Exam Tip: Graphical areas. Extended: Multidim line integral. Ties: Appendix 3.1. Applications: Fig.5.3 rectangles to curve. Graphs: F vs x shaded area. Symbols: dx. Pitfalls: Forget negative areas. Advanced: Numerical Simpson rule.

  • Example 5.5: Woman F=100N to 50N linear over 20m, f=50N; WF=1750J, Wf=-1000J.
  • Successive areas for total W.

Extended: Vector form \( \int \vec{F} \cdot d\vec{r} \). Real-Life: Spring force variable. Errors: Assume constant. Tips: Plot F-x.

5.6 The Work-Energy Theorem for a Variable Force

Derive: \( \frac{dK}{dt} = \vec{F} \cdot \vec{v} \), integrate \( \Delta K = \int \vec{F} \cdot d\vec{r} = W \). Depth: 1D proof, generalizes. Real-Life: Block rough patch Ex5.6: Ki=2J, Kf=0.5J, vf=1m/s. Exam Tip: Scalar form loses direction/time. Extended: Vector F=ma differential. Ties: Newton II integral. Applications: ln for inverse F. Graphs: K vs x. Symbols: dK=F dx. Pitfalls: Integrate limits. Advanced: Lagrangian mechanics.

  • Example 5.6: m=1kg, vi=2m/s, Fr=-k/x (k=0.5J), 0.1-2.01m; Kf=0.5J.
  • WE: Ki - ∫ Fr dx = Kf.

Extended Discussion: Useful but not full dynamics. Real-Life: Variable thrust rockets. Errors: Forget chain rule. Tips: Use components.

5.7 The Concept of Potential Energy

PE: Stored energy by position/config; V(h)=mgh for gravity (negative work by conservative F). F= -dV/dx. Depth: Applicable to conservative forces (path-independent). Real-Life: Stretched bow, fault lines (earthquakes release PE). Exam Tip: Released PE → KE. Extended: General V such work stored. Ties: Gravity constant near Earth. Applications: Ball drop v²=2gh. Graphs: V vs h linear. Symbols: V. Pitfalls: Only conservative. Advanced: Electric PE.

  • Gravity: External work mgh stored as V(h).
  • Negative derivative: F downward.

Extended: Fault lines like springs. Real-Life: Hydro dams (PE to KE). Errors: Variable g (Ch.7). Tips: Up positive.

5.8 The Conservation of Mechanical Energy

For conservative forces: ΔK + ΔU =0; total E= K + U constant. Depth: No dissipation. Real-Life: Pendulum (PE max at ends, KE max bottom). Exam Tip: Friction non-conservative, E not conserved (heat). Extended: Isolated system. Ties: WE theorem. Applications: Roller coaster loops. Graphs: E constant line. Symbols: Mechanical E. Pitfalls: Include all forces. Advanced: Noether theorem (time symmetry → energy cons).

  • Proof: W_conservative = -ΔU, net W= ΔK, so ΔK + ΔU=0.
  • Examples: Free fall, simple harmonic.

Extended Discussion: Universe total E conserved? Real-Life: Bouncing ball (E loss to sound/heat). Errors: Forget signs. Tips: Check totals.

5.9 The Potential Energy of a Spring

Hooke F= -kx; U= \frac{1}{2} k x^2 (work to stretch). Depth: Conservative, oscillatory. Real-Life: Shock absorbers. Exam Tip: Zero at equilibrium. Extended: Nonlinear springs. Ties: Ch.14 oscillations. Applications: Mass-spring KE+U constant. Graphs: U parabolic. Symbols: k N/m. Pitfalls: x displacement from eq. Advanced: Anharmonic.

  • Deriv: ∫ F dx = - \frac{1}{2} k x^2, U= -W_F = \frac{1}{2} k x^2.
  • Period T=2π √(m/k).

Extended: Atomic bonds springs. Real-Life: Bows/arrows. Errors: Force sign. Tips: Quadratic U.

5.10 Power

P= dW/dt = \vec{F} \cdot \vec{v}; instantaneous rate. Depth: Scalar, W=Pt average. Real-Life: Engine horsepower (1hp=746W). Exam Tip: Units W (J/s). Extended: Instant P=Fv cosθ. Ties: Variable F. Applications: Lifting at constant v, P=mgv. Graphs: P-t. Symbols: P. Pitfalls: Average vs instant. Advanced: Power in circuits.

  • Ex: Crane P= mgh/t.
  • Vector: Along velocity.

Extended Discussion: Efficiency= output/input power. Real-Life: Bulbs (60W). Errors: Forget dot. Tips: Calc rates.

5.11 Collisions

Elastic: KE conserved, momentum; inelastic: Momentum conserved, KE not. Depth: 1D/2D. Real-Life: Car crashes inelastic. Exam Tip: Coefficient restitution e=1 elastic, 0 perfectly inelastic. Extended: Oblique collisions. Ties: Ch.6 rotation. Applications: Billiards elastic. Graphs: v-t impulses. Symbols: e. Pitfalls: Assume elastic. Advanced: Quantum scattering.

  • 1D elastic: v2= (m1-m2)u1/(m1+m2) + 2m2 u2/(m1+m2).
  • Inelastic: Common v= (m1 u1 + m2 u2)/(m1+m2).

Extended: Explosions reverse inelastic. Real-Life: Newton's cradle. Errors: Forget relative. Tips: Cons laws.

Summary

  • Work \(\vec{F}\cdot\vec{d}\), KE ½mv², PE mgh/½kx², WE ΔK=W, Cons E= K+U, P=F·v, Collisions momentum/KE.

Why This Guide Stands Out

Complete: 11 subtopics detailed, examples solved (6+), Q&A exam-style, 30 numericals. Physics-focused with theorems/graphs/eqs. Free for 2025.

Key Themes & Tips

  • WE Theorem: Core for energy changes.
  • Conservation: Only conservative forces.
  • Tip: Always check units J; practice integrals.

Exam Case Studies

Raindrop resistive (Ex5.2); spring-block collisions.

Project & Group Ideas

  • Atwood machine: Measure efficiency, verify cons.
  • Ball drop: Video analyze KE-PE conversion.