This MCQ module is based on: NCERT Exercises and Solutions: Work, Energy and Power
NCERT Exercises and Solutions: Work, Energy and Power
This assessment will be based on: NCERT Exercises and Solutions: Work, Energy and Power
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NCERT Exercises and Solutions: Work, Energy and Power
Chapter 5 — Summary
- Scalar product: \(\vec{A}\cdot\vec{B} = AB\cos\theta = A_xB_x + A_yB_y + A_zB_z\)
- Work (constant force): \(W = \vec{F}\cdot\vec{d} = Fd\cos\theta\)
- Work (variable force): \(W = \int F(x)\,dx\) — area under F-x curve
- Kinetic energy: \(K = \tfrac{1}{2}mv^2\)
- Work-Energy Theorem: \(W_{\text{net}} = \Delta K\)
- Gravitational PE (near Earth): \(V = mgh\)
- Spring PE: \(V = \tfrac{1}{2}kx^2\)
- Conservation of mechanical energy: \(E = K + V = \text{const}\) (only conservative forces)
- Power (avg): \(P_{\text{avg}} = W/t\); (inst): \(P = \vec{F}\cdot\vec{v}\)
- Elastic 1D (m₂ at rest): \(v_1 = \frac{m_1-m_2}{m_1+m_2}u_1\), \(v_2 = \frac{2m_1}{m_1+m_2}u_1\)
- Perfectly inelastic: \(v = \frac{m_1u_1+m_2u_2}{m_1+m_2}\); KE always lost
| Quantity | SI Unit | Dimensions |
|---|---|---|
| Work / Energy | J (joule) | [ML²T⁻²] |
| Kinetic Energy | J | [ML²T⁻²] |
| Potential Energy | J | [ML²T⁻²] |
| Power | W (watt) = J/s | [ML²T⁻³] |
| Force | N | [MLT⁻²] |
| Spring constant k | N/m | [MT⁻²] |
🎯 Quick Self-Check Calculator
Try a quick KE calculation. Enter mass and speed; the calculator returns kinetic energy and equivalent work needed to bring the body to rest.
NCERT Exercises — Worked Solutions
Exercise 5.1: Sign of Work
The sign of work done by a force on a body is important to understand. State carefully if the following quantities are positive, negative or zero:
(a) work done by a man in lifting a bucket out of a well by means of a rope tied to the bucket.
(b) work done by gravitational force in the above case.
(c) work done by friction on a body sliding down an inclined plane.
(d) work done by an applied force on a body moving on a rough horizontal plane with uniform velocity.
(e) work done by the resistive force of air on a vibrating pendulum in bringing it to rest.
(b) Negative: Gravity acts downward; bucket moves upward — opposite directions.
(c) Negative: Friction always opposes motion (180° to displacement).
(d) Positive: Applied force is in direction of motion (otherwise the body could not maintain uniform velocity against friction).
(e) Negative: Air resistance always opposes velocity.
Exercise 5.2: Work and Friction
A body of mass 2 kg initially at rest moves under the action of an applied horizontal force of 7 N on a table with coefficient of kinetic friction = 0.1. Compute (a) work done by the applied force in 10 s, (b) work done by friction in 10 s, (c) work done by the net force on the body in 10 s, (d) change in kinetic energy of the body in 10 s, and interpret your results.
Net force = 7 − 1.96 = 5.04 N. Acceleration a = 5.04/2 = 2.52 m/s².
Distance in 10 s: s = ½at² = ½(2.52)(100) = 126 m. Final speed v = at = 25.2 m/s.
(a) W_applied = 7 × 126 = 882 J.
(b) W_friction = −1.96 × 126 = −246.96 J (≈ −247 J).
(c) W_net = 5.04 × 126 = 635.04 J (≈ 635 J).
(d) ΔK = ½(2)(25.2)² − 0 = 635.04 J. Matches W_net — confirms work-energy theorem.
Exercise 5.3: Potential Energy from F(x)
Given F(x) for 0 ≤ x ≤ a as F = +F₀ and for a ≤ x ≤ 2a as F = −F₀ (a step force), sketch V(x) given V(0) = 0.
For 0 ≤ x ≤ a: V = −F₀x (decreases linearly to V = −F₀a at x = a).
For a ≤ x ≤ 2a: V = −F₀a + F₀(x − a) = F₀(x − 2a) (rises linearly back to V = 0 at x = 2a).
Shape: V is V-shaped with minimum at x = a, value −F₀a; symmetric about x = a.
Exercise 5.4: Power & Lifting
An electric motor of power 5 kW is used to lift water out of a 50 m deep well. How much water in litres can it lift in one hour? (g = 9.8 m/s², density of water = 1000 kg/m³)
For mass m of water, mgh = energy ⇒ m = E/(gh) = 1.8 × 10⁷/(9.8 × 50) ≈ 36 735 kg.
Volume = m/ρ = 36 735/1000 = 36.735 m³ = 36 735 L.
(Realistically, motors are not 100% efficient — actual lift would be ~70% of this.)
Exercise 5.5: Spring & Energy
A spring of force constant 1200 N/m is mounted on a horizontal table. A 3 kg block is pushed against the spring, compressing it by 2.0 cm. Then released. Find the speed of the block when the spring reaches its natural length. (frictionless surface)
At natural length all of this is KE: ½(3)v² = 0.24 ⇒ v² = 0.16 ⇒ v = 0.40 m/s.
Exercise 5.6: Conservative Field
State if each of the following statements is true or false. Give reasons.
(a) The total energy of a system is always conserved if all forces are conservative.
(b) Work done by a conservative force on a particle in a closed loop is always zero.
(c) Total mechanical energy of a system is conserved if external and conservative forces act on it.
(d) In an inelastic collision, the final KE is always less than initial KE.
(b) True. By definition of conservative force.
(c) Partially true. Conservative forces do; external forces may add or remove energy. Strictly the statement as given would require external forces to do net zero work.
(d) True. Inelastic by definition has KE loss.
Exercise 5.7: Work in Various Cases
State if each is true or false:
(a) Work done by static friction is always zero.
(b) The kinetic energy of a body is always non-negative.
(c) An object can have zero velocity and still have non-zero acceleration.
(d) Two satellites of equal mass orbiting at different altitudes have the same KE.
(b) True. K = ½mv² ≥ 0.
(c) True. A ball at the top of its toss has v = 0 but a = g.
(d) False. KE depends on orbital speed, which decreases with altitude (for circular orbits, v² ∝ 1/r).
Exercise 5.8: Variable-Force Work
A particle of mass 0.5 kg is acted on by a force F(x) = (3 + 2x) N along the +x axis, where x is in metres. Find the work done from x = 0 to x = 4 m, and the speed at x = 4 m if it started from rest.
Exercise 5.9: Elastic Collision Mass Ratio
A 4 kg ball moving at 10 m/s collides elastically head-on with a 6 kg ball at rest. Find post-collision velocities and KE of each ball.
Trace the energy path in each scenario: identify whether energy is converted between K, V, or lost as heat/light.
- A pendulum swinging in air gradually loses amplitude.
- A coin spinning on a table eventually stops.
- A bouncing ball rebounds to lower height each time.
- An orbiting satellite has constant total mechanical energy.
- Pendulum: K↔V cycles, but air drag converts mechanical → thermal energy of air.
- Coin: Rotational K → heat (friction with table) + sound.
- Ball: Each bounce converts some KE to internal heat/sound; height decreases as energy budget shrinks.
- Satellite: Constant E because gravity is conservative and air drag is negligible at orbital altitudes.
The "graveyard" of all dissipation is thermal energy (random molecular motion) — the second law of thermodynamics in action.
🎯 Competency-Based Questions
Q1. What kind of force is friction here?L1 Remember
Q2. Distance travelled before stopping?L3 Apply
Q3. Heat generated by friction over this distance?L3 Apply
Q4. State whether TRUE or FALSE: "If the surface were frictionless and there were no air drag, the block would slide forever at 5 m/s." L5 Evaluate
Q5. HOT: The same block is fired at 5 m/s up a 30° incline (same μ). Will it travel further or shorter than 6.25 m? Justify quantitatively. L6 Create
🧠 Assertion–Reason Questions
Choose: (A) Both true, R explains A. (B) Both true, R does NOT explain A. (C) A true, R false. (D) A false, R true.
Assertion (A): Energy can never be created or destroyed.
Reason (R): The total energy of an isolated system is conserved (first law of thermodynamics).
Assertion (A): A heavy car has more KE than a light bicycle even at the same speed.
Reason (R): KE is directly proportional to mass.
Assertion (A): When a body is in equilibrium, no work is done on it.
Reason (R): Net force on a body in equilibrium is zero.