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Study Guide: Physics Mechanics - How to Solve: Conservation of Linear Momentum (Explosions, Recoil, Bullet-Block System) – IIT JEE Guide
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Physics Mechanics - How to Solve: Conservation of Linear Momentum (Explosions, Recoil, Bullet-Block System) – IIT JEE Guide

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

⏱️ ~7 min read

How to Solve: Conservation of Linear Momentum (Explosions, Recoil, Bullet-Block System) – IIT JEE Guide

Introduction

Mastering conservation of linear momentum in explosions, recoil, and bullet-block systems unlocks 5-8 marks in IIT JEE (Main + Advanced)—enough to push you into the top 10%. Whether it’s a gun firing a bullet, a bomb splitting into fragments, or a block absorbing a bullet, this concept appears every year. Miss it, and you lose easy marks. Nail it, and you solve problems in under 2 minutes.

WHAT YOU NEED TO KNOW FIRST

Before diving in, ensure you understand:
1. Newton’s 3rd Law – Action-reaction forces are equal and opposite.
2. Definition of Linear Momentum (p = mv) – Momentum is mass × velocity.
3. Vector Nature of Momentum – Direction matters; assign signs (+/-) to velocities.

If any of these are unclear, stop and review them first.

KEY TERMS & FORMULAS

Key Terms

  1. System – The objects we’re studying (e.g., gun + bullet, bomb + fragments).
  2. External Force – A force acting on the system from outside (e.g., gravity, friction).
  3. Internal Force – Forces between objects inside the system (e.g., explosion force, recoil).
  4. Conservation of Momentum – If no external force acts, the total momentum before = total momentum after.

Formulas

  1. Momentum of a Single Object [ p = mv ]
  2. ( p ) = momentum (kg·m/s)
  3. ( m ) = mass (kg)
  4. ( v ) = velocity (m/s)
  5. MEMORISE THIS

  6. Conservation of Linear Momentum (1D) [ m_1u_1 + m_2u_2 = m_1v_1 + m_2v_2 ]

  7. ( u ) = initial velocity (before event)
  8. ( v ) = final velocity (after event)
  9. MEMORISE THIS (Given on JEE sheet, but know how to apply it)

  10. Conservation of Momentum (2D – Vector Form) [ \vec{p}{\text{initial}} = \vec{p} ]}

  11. Break into x and y components if needed.
  12. MEMORISE THIS APPROACH

STEP-BY-STEP METHOD

Follow these exact steps for every momentum conservation problem.

Step 1: Define the System

  • Circle all objects involved (e.g., gun + bullet, bomb + fragments).
  • Check for external forces:
  • If no external force (or negligible), momentum is conserved.
  • If external force exists (e.g., friction, gravity), momentum is not conserved (unless the force is perpendicular to motion).

Step 2: Assign Directions & Signs

  • Choose a positive direction (e.g., right = +, left = –).
  • All velocities must have signs (+ or –).

Step 3: Write Initial & Final Momentum

  • Initial Momentum (Before Event):
  • Sum of momenta of all objects before the event (e.g., explosion, firing).
  • If objects are at rest, initial momentum = 0.
  • Final Momentum (After Event):
  • Sum of momenta of all objects after the event.

Step 4: Apply Conservation of Momentum

[ \text{Initial Momentum} = \text{Final Momentum} ] - Plug in values with correct signs. - Solve for the unknown.

Step 5: Check Units & Reasonableness

  • Ensure all masses are in kg, velocities in m/s.
  • Does the answer make sense? (e.g., lighter object should move faster).

WORKED EXAMPLES

Example 1 – Basic (Gun Firing a Bullet)

Problem: A 2 kg gun fires a 0.01 kg bullet at 200 m/s. What is the recoil velocity of the gun?

Solution (Step-by-Step):

  1. Define the System:
  2. Objects: Gun + bullet.
  3. No external force (friction neglected) → Momentum conserved.

  4. Assign Directions:

  5. Let bullet’s direction = +x.
  6. Gun’s recoil = –x (opposite direction).

  7. Initial Momentum:

  8. Gun and bullet at rest → Initial momentum = 0.

  9. Final Momentum:

  10. Bullet: ( p_{\text{bullet}} = m_{\text{bullet}} \times v_{\text{bullet}} = 0.01 \times 200 = +2 \, \text{kg·m/s} )
  11. Gun: ( p_{\text{gun}} = m_{\text{gun}} \times v_{\text{gun}} = 2 \times v_{\text{gun}} ) (negative, since recoil is opposite)

  12. Apply Conservation: [ 0 = p_{\text{bullet}} + p_{\text{gun}} ] [ 0 = 2 + 2v_{\text{gun}} ] [ v_{\text{gun}} = -1 \, \text{m/s} ]

  13. Negative sign means gun moves opposite to bullet.

  14. Check:

  15. Gun is 200× heavier → moves 200× slower (1 m/s vs 200 m/s). Makes sense!

What we did and why: - Used conservation of momentum because no external force acted. - Assigned signs to velocities to account for direction. - Solved for recoil velocity by equating initial and final momenta.

Example 2 – Medium (Explosion into Two Fragments)

Problem: A 5 kg bomb at rest explodes into two fragments: - Fragment A: 2 kg, moves at 30 m/s at 30° above horizontal. - Fragment B: 3 kg, moves at unknown speed at θ below horizontal. Find the speed of Fragment B.

Solution (Step-by-Step):

  1. Define the System:
  2. Objects: Fragment A + Fragment B.
  3. No external force → Momentum conserved.

  4. Assign Directions:

  5. Let horizontal = +x, vertical = +y.
  6. Initial momentum = 0 (bomb at rest).

  7. Break into Components:

  8. Fragment A (2 kg, 30 m/s, 30°):
    • ( p_{Ax} = 2 \times 30 \cos 30° = 2 \times 30 \times \frac{\sqrt{3}}{2} = 30\sqrt{3} \, \text{kg·m/s} )
    • ( p_{Ay} = 2 \times 30 \sin 30° = 2 \times 30 \times 0.5 = 30 \, \text{kg·m/s} )
  9. Fragment B (3 kg, v, θ):

    • ( p_{Bx} = 3v \cos θ )
    • ( p_{By} = -3v \sin θ ) (negative because it’s below horizontal)
  10. Apply Conservation (x and y separately):

  11. x-direction: [ 0 = p_{Ax} + p_{Bx} \implies 0 = 30\sqrt{3} + 3v \cos θ ] [ 3v \cos θ = -30\sqrt{3} \quad (1) ]
  12. y-direction: [ 0 = p_{Ay} + p_{By} \implies 0 = 30 - 3v \sin θ ] [ 3v \sin θ = 30 \quad (2) ]

  13. Solve for v:

  14. Divide (2) by (1): [ \frac{3v \sin θ}{3v \cos θ} = \frac{30}{-30\sqrt{3}} \implies \tan θ = -\frac{1}{\sqrt{3}} ] [ θ = 150° \text{ or } -30° \quad (\text{We take } θ = 30° \text{ below horizontal}) ]
  15. Plug ( θ = 30° ) into (2): [ 3v \sin 30° = 30 \implies 3v \times 0.5 = 30 \implies v = 20 \, \text{m/s} ]

  16. Check:

  17. Fragment B is heavier → moves slower (20 m/s vs 30 m/s). Makes sense!

What we did and why: - Used vector conservation (x and y components) because explosion was 2D. - Solved two equations to find speed and angle. - Verified that heavier fragment moves slower.

Example 3 – Exam-Style (Bullet-Block System with Friction)

Problem (JEE Advanced 2018-Style): A 0.01 kg bullet moving at 500 m/s hits a 2 kg block at rest on a rough surface (μ = 0.2). The bullet embeds in the block. How far does the block slide before stopping?

Solution (Step-by-Step):

  1. Define the System:
  2. Objects: Bullet + block.
  3. External force = friction → Momentum not conserved during collision.
  4. But: During collision (instantaneous), friction is negligible → Momentum conserved for collision only.

  5. Step 1: Find Velocity After Collision (Momentum Conservation)

  6. Initial momentum = ( 0.01 \times 500 + 2 \times 0 = 5 \, \text{kg·m/s} )
  7. Final momentum = ( (0.01 + 2) \times v = 2.01v )
  8. Apply conservation: [ 5 = 2.01v \implies v = \frac{5}{2.01} \approx 2.49 \, \text{m/s} ]

  9. Step 2: Find Stopping Distance (Work-Energy Principle)

  10. Friction force = ( μmg = 0.2 \times 2.01 \times 9.8 \approx 3.94 \, \text{N} )
  11. Work done by friction = ( F \times d )
  12. Initial KE = ( \frac{1}{2} \times 2.01 \times (2.49)^2 \approx 6.23 \, \text{J} )
  13. Work-Energy Theorem: [ W = ΔKE \implies -3.94d = 0 - 6.23 ] [ d = \frac{6.23}{3.94} \approx 1.58 \, \text{m} ]

  14. Check:

  15. Bullet embeds → inelastic collision → KE not conserved, but momentum is (during collision).
  16. Friction after collision slows the block.

What we did and why: - Split the problem into collision (momentum conserved) and post-collision (friction acts). - Used work-energy principle to find stopping distance. - Exam trap: If you applied momentum conservation after collision, you’d get the wrong answer.

COMMON MISTAKES

MISTAKE WHY IT HAPPENS CORRECT APPROACH
Ignoring signs (+/-) for velocities Forgetting that momentum is a vector Always assign positive/negative directions before solving.
Applying momentum conservation when external forces act Assuming momentum is always conserved Check for external forces (e.g., friction, gravity). If present, momentum is not conserved.
Using kinetic energy instead of momentum Confusing elastic vs inelastic collisions In explosions/recoil, momentum is conserved, but KE is not.
Forgetting to include all objects in the system Missing a fragment or object Circle all objects in the problem before writing equations.
Mixing up initial and final states Writing momentum equations incorrectly Before event = After event (e.g., before explosion = after explosion).

EXAM TRAPS

TRAP HOW TO SPOT IT HOW TO AVOID IT
External forces (e.g., friction) acting during collision Problem mentions a rough surface or gravity Momentum is conserved only during the collision (instantaneous). After collision, use work-energy or kinematics.
2D explosions (fragments at angles) Problem gives angles or asks for direction Break into x and y components and solve separately.
Bullet-block system with friction Bullet embeds in block, and surface is not smooth First conserve momentum (collision), then use work-energy (post-collision).

1-MINUTE RECAP (Night Before Exam)

"Listen up—this is how you own momentum problems in JEE:

  1. System first: Circle all objects. If no external force, momentum is conserved.
  2. Signs matter: Assign + and – to velocities. Left = –, right = +.
  3. Initial = Final: Write ( m_1u_1 + m_2u_2 = m_1v_1 + m_2v_2 ). If at rest, initial momentum = 0.
  4. 2D? Break into x and y. Solve each component separately.
  5. Bullet-block? First collision (momentum conserved), then post-collision (work-energy).
  6. Check units: kg, m/s. Does the answer make sense? Heavier object = slower speed.

You’ve got this. Now go solve those 5-8 marks like a pro."