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Study Guide: Physics Mechanics - How to Solve: Combined Translation and Rotation (Rolling on Incline, Angular Impulse) – IIT JEE Guide
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Physics Mechanics - How to Solve: Combined Translation and Rotation (Rolling on Incline, Angular Impulse) – IIT JEE Guide

By Fatskills Exam Guides Team — the exam nerds behind 28,500+ quizzes and 2.1M practice questions across 500+ global exams.

⏱️ ~6 min read

How to Solve: Combined Translation and Rotation (Rolling on Incline, Angular Impulse) – IIT JEE Guide

Introduction

Mastering rolling motion and angular impulse can get you 10–15 marks in IIT JEE—enough to push you into the top 1000 ranks. From a rolling wheel on a hill to a cricket ball skidding before rolling, this concept appears in every mechanics problem where objects both move and spin.

WHAT YOU NEED TO KNOW FIRST

Before diving in, ensure you’re rock-solid on:
1. Newton’s Second Law (F = ma) – For linear motion.
2. Torque and Angular Acceleration (τ = Iα) – For pure rotation.
3. Kinetic Energy of Rolling (K = ½mv² + ½Iω²) – For energy conservation.

If any of these feel shaky, stop now and review them first.

KEY TERMS & FORMULAS

1. Pure Rolling Condition (No Slipping)

Formula: v = rω (Linear velocity = radius × angular velocity) - v = linear velocity of the center of mass (m/s) - r = radius of the rolling object (m) - ω = angular velocity (rad/s) MEMORISE THIS – This is the golden rule of rolling motion.

2. Acceleration of a Rolling Object on an Incline

Formula: a = g sinθ / (1 + I/mr²) - a = linear acceleration of the center of mass (m/s²) - g = acceleration due to gravity (9.8 m/s²) - θ = angle of incline (degrees or radians) - I = moment of inertia about the center of mass (kg·m²) - m = mass of the object (kg) - r = radius (m) MEMORISE THIS – Derived from energy or torque methods.

3. Moment of Inertia (Common Shapes)

Object Moment of Inertia (I) MEMORISE
Solid sphere (2/5)mr²
Hollow sphere (2/3)mr²
Solid cylinder (1/2)mr²
Hollow cylinder mr²
Thin rod (center) (1/12)ml²

4. Angular Impulse (Change in Angular Momentum)

Formula: J = ΔL = IΔω = τΔt - J = angular impulse (N·m·s or kg·m²/s) - ΔL = change in angular momentum (kg·m²/s) - I = moment of inertia (kg·m²) - Δω = change in angular velocity (rad/s) - τ = torque (N·m) - Δt = time interval (s) Given on exam sheet – But you must know how to apply it.

5. Work-Energy Theorem for Rolling

Formula: Work done = ΔK = ½mv² + ½Iω² - K = total kinetic energy (J) - ½mv² = translational KE - ½Iω² = rotational KE MEMORISE THIS – Critical for energy-based problems.

STEP-BY-STEP METHOD

Problem Type 1: Rolling on an Incline (No Slipping)

Steps:
1. Draw a free-body diagram (FBD). - Weight (mg) acting downward. - Normal force (N) perpendicular to the incline. - Friction (f) acting up the incline (prevents slipping).
2. Write Newton’s Second Law for translation. - Along the incline: mg sinθ – f = ma - Perpendicular to incline: N = mg cosθ
3. Write torque equation for rotation. - Torque due to friction: τ = f × r = Iα - Relate α to a: α = a/r (from pure rolling condition)
4. Substitute α into torque equation. - f × r = I × (a/r) - f = Ia/r²
5. Substitute f into Newton’s equation. - mg sinθ – (Ia/r²) = ma - a = g sinθ / (1 + I/mr²)
6. Plug in the moment of inertia (I) for the given shape. - Example: For a solid sphere, I = (2/5)mr² - a = g sinθ / (1 + (2/5)) = (5/7)g sinθ

Problem Type 2: Angular Impulse (Change in Angular Momentum)

Steps:
1. Identify the torque (τ) and time (Δt). - If torque is constant: J = τΔt - If torque varies: J = ∫τ dt (rare in JEE)
2. Relate impulse to change in angular momentum. - J = ΔL = IΔω
3. Find initial and final angular velocities (ω₁, ω₂). - If the object starts from rest: ω₁ = 0
4. Solve for the unknown (I, ω, or τ). - Example: If J = 10 N·m·s and I = 2 kg·m², then Δω = J/I = 5 rad/s

WORKED EXAMPLES

Example 1 – Basic: Rolling Sphere on Incline

Problem: A solid sphere of mass 2 kg and radius 0.1 m rolls down a 30° incline without slipping. Find its acceleration.

Solution:
1. FBD: Weight (mg), normal (N), friction (f) up the incline.
2. Newton’s Law (translation): - mg sinθ – f = ma - 2 × 9.8 × sin30° – f = 2a - 9.8 – f = 2a (Equation 1)
3. Torque equation (rotation): - τ = f × r = Iα - f × 0.1 = (2/5 × 2 × 0.1²) × (a/0.1) - f = (0.008) × (a/0.1) = 0.08a (Equation 2)
4. Substitute f from Equation 2 into Equation 1: - 9.8 – 0.08a = 2a - 9.8 = 2.08a - a = 9.8 / 2.08 ≈ 4.71 m/s²
5. Check with formula: - a = g sinθ / (1 + I/mr²) = 9.8 × 0.5 / (1 + 0.4) = 4.9 / 1.4 ≈ 3.5 m/s² (Oops! Mistake spotted—corrected below.)

Correction: - I = (2/5)mr² = (2/5) × 2 × 0.01 = 0.008 kg·m² - I/mr² = 0.008 / (2 × 0.01) = 0.4 - a = 9.8 × 0.5 / (1 + 0.4) = 4.9 / 1.4 = 3.5 m/s²

What we did and why: - Used Newton’s Law + Torque to relate linear and angular motion. - Applied the pure rolling condition (v = rω) to connect a and α. - Always check with the formula to avoid arithmetic errors.

Example 2 – Medium: Angular Impulse on a Rod

Problem: A uniform rod of mass 3 kg, length 2 m, is pivoted at one end. A force of 10 N is applied perpendicular to the rod at the other end for 0.5 s. Find the angular velocity acquired.

Solution:
1. Moment of inertia (rod about end): - I = (1/3)ml² = (1/3) × 3 × 4 = 4 kg·m²
2. Torque (τ): - τ = F × r = 10 × 2 = 20 N·m
3. Angular impulse (J): - J = τΔt = 20 × 0.5 = 10 N·m·s
4. Change in angular momentum (ΔL): - J = ΔL = IΔω - 10 = 4 × Δω - Δω = 2.5 rad/s

What we did and why: - Used angular impulse = change in angular momentum. - Calculated I for a rod pivoted at one end. - No linear motion here—only rotation about the pivot.

Example 3 – Exam-Style: Rolling + Slipping to Pure Rolling

Problem: A hollow cylinder of mass 4 kg, radius 0.2 m, is given an initial linear velocity v₀ = 6 m/s on a rough horizontal surface. The coefficient of friction is μ = 0.3. Find: (a) Time taken to start pure rolling. (b) Final velocity when pure rolling begins.

Solution:
1. Friction force (f): - f = μmg = 0.3 × 4 × 9.8 = 11.76 N
2. Linear deceleration (a): - f = ma → a = f/m = 11.76 / 4 = 2.94 m/s²
3. Angular acceleration (α): - τ = f × r = Iα - I = mr² (hollow cylinder) = 4 × 0.04 = 0.16 kg·m² - 11.76 × 0.2 = 0.16 × α → α = 14.7 rad/s²
4. Time to pure rolling (v = rω): - v = v₀ – at - ω = αt - v = rω → v₀ – at = r(αt) - 6 – 2.94t = 0.2 × 14.7t - 6 = 2.94t + 2.94t = 5.88t - t = 6 / 5.88 ≈ 1.02 s
5. Final velocity (v): - v = v₀ – at = 6 – 2.94 × 1.02 ≈ 3 m/s

What we did and why: - Friction causes both linear deceleration and angular acceleration. - Pure rolling starts when v = rω. - Used kinematic equations for both linear and angular motion.

COMMON MISTAKES

MISTAKE WHY IT HAPPENS CORRECT APPROACH
Ignoring friction direction Students assume friction acts down the incline. Friction opposes slipping—for rolling down, it acts up the incline.
Using wrong moment of inertia Confusing solid vs. hollow shapes. Memorise I for common shapes (sphere, cylinder, rod).
Forgetting pure rolling condition (v = rω) Solving translation and rotation separately. Always relate v and ω in rolling problems.
Mixing up linear and angular acceleration Using a = αr incorrectly. a = αr only if no slipping—otherwise, they’re independent.
Assuming energy is conserved in slipping Forgetting friction does work. Energy is lost when slipping occurs—use work-energy carefully.

EXAM TRAPS

TRAP HOW TO SPOT IT HOW TO AVOID IT
Disguised pure rolling condition Problem says "starts rolling without slipping" but doesn’t mention v = rω. Always check if v = rω applies—if yes, use it.
Variable torque in angular impulse Problem gives a time-varying force (e.g., F = kt). Integrate τ = r × F over time to find impulse.
Non-uniform mass distribution Problem mentions a rod with a mass at one end. Calculate I using parallel axis theorem if needed.

1-MINUTE RECAP (Night Before Exam)

"Listen up—this is your 60-second crash course on rolling and angular impulse for JEE.

  1. Pure rolling = v = rω. If it’s rolling without slipping, this is your lifeline.
  2. Acceleration on an incline? Use a = g sinθ / (1 + I/mr²). Plug in I for the shape.
  3. Angular impulse? J = τΔt = IΔω. If torque is constant, it’s just τ × time.
  4. Slipping to rolling? Friction causes linear deceleration and angular acceleration—set v = rω to find time.
  5. Energy? K = ½mv² + ½Iω². But if slipping happens, energy isn’t conserved—friction does work.

Last tip: If you see a wheel, sphere, or cylinder on a slope, draw the FBD first. Friction acts up the incline—never forget that.

Now go crush that exam.