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Newton’s Third Law, Momentum and Conservation of Momentum

🎓 Class 9 Science CBSE Theory Ch 6 — How Forces Affect Motion ⏱ ~13 min
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This MCQ module is based on: Newton’s Third Law, Momentum and Conservation of Momentum

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6.8 Newton's Third Law of Motion

If you have ever stepped off a small boat onto a jetty, you may have felt the boat slide backward as you stepped forward. Why does that happen? You exerted a force on the boat through your foot — and the boat exerted an equal and opposite force on you. This mutual interaction is the heart of Newton's Third Law.

Newton's Third Law of Motion: To every action, there is an equal and opposite reaction. Forces always occur in pairs — if body A exerts a force on body B, body B simultaneously exerts an equal force on body A in the opposite direction.

Two key features of action–reaction pairs:

  • They are equal in magnitude and opposite in direction.
  • They act on two different bodies — never on the same body. (That is why they do not cancel out the way balanced forces do.)

Examples of action–reaction pairs

  • Walking: Your foot pushes the ground backward (action). The ground pushes your foot forward with an equal force (reaction). That is what propels you ahead.
  • Swimmer: A swimmer pushes the water backward with the hands; the water pushes the swimmer forward.
  • Rocket launch: Hot gases are expelled downward at high speed (action). The gases push the rocket upward (reaction).
  • Recoil of a gun: When a gun fires, the gun pushes the bullet forward, and the bullet pushes the gun back. The gun is felt as a "kick" on the shoulder.
  • Jumping off a boat: The person pushes the boat backward; the boat pushes the person forward toward the shore.

🚶🚀 Action–Reaction Pairs — Compare two scenes L4 Analyse

Newton's Third Law lives in both an everyday walk and a giant rocket launch. Click each scene and analyse: which body is the action acting on, and which body is the reaction acting on?

Walking Reaction (forward) Action (backward) Rocket Launch Action (gases ↓) Reaction (rocket ↑)
Fig 6.6: Action–reaction pairs in walking and rocket launch.
Click either the walker or the rocket above to analyse the action–reaction pair.

6.9 Momentum

If a fast-moving cricket ball hits you, it hurts more than a slow-moving one of the same mass. A heavy lorry at 5 m/s causes more damage in a collision than a bicycle at 5 m/s. Both mass and velocity matter when describing the "quantity of motion" of a body. Newton combined the two into a single quantity called momentum.

Momentum: \(p = m v\). Momentum is a vector quantity — its direction is the same as that of the velocity. Its SI unit is kg·m/s.

Change in momentum

If a body's velocity changes from \(u\) to \(v\) in a time \(t\), the change in momentum is \(\Delta p = mv - mu = m(v-u)\). This is closely linked to the Second Law:

\(F = m a = m \dfrac{v-u}{t} = \dfrac{m v - m u}{t} = \dfrac{\Delta p}{t}\)

So Newton's Second Law can also be stated as: the rate of change of momentum of a body is equal to the net force acting on it.

Impulse

Multiplying both sides of \(F = \Delta p/t\) by \(t\) gives:

Impulse: \(F \cdot t = \Delta p\)

Impulse measures the total effect of a force acting for a time \(t\). The same change in momentum can be produced by a large force for a short time or a small force for a long time. That is why we bend our knees on landing from a jump (longer \(t\) → smaller \(F\)) and why a cricketer pulls the hands back while catching a fast ball.

6.10 Law of Conservation of Momentum

Consider two bodies that interact only with each other (an "isolated system" — no external forces). Newton's Third Law guarantees that whatever force one exerts on the other is exactly cancelled by the equal and opposite force on itself. The result is one of the deepest laws in physics:

Law of Conservation of Momentum: The total momentum of an isolated system of bodies remains constant if no external unbalanced force acts on it.

If two bodies of masses \(m_1\) and \(m_2\) have initial velocities \(u_1\) and \(u_2\), and after they interact the velocities become \(v_1\) and \(v_2\), then:

\(m_1 u_1 + m_2 u_2 = m_1 v_1 + m_2 v_2\)

Recoil of a gun — a textbook application

Example 1 — Recoil velocity of a gun

Q. A gun of mass 4 kg fires a bullet of mass 20 g with a velocity of 200 m/s. Find the recoil velocity of the gun.

Solution. Mass of bullet \(m_1 = 0.020\) kg, velocity \(v_1 = 200\) m/s. Mass of gun \(m_2 = 4\) kg, recoil velocity \(v_2 = ?\). Initially both are at rest, so total initial momentum is 0.

By conservation of momentum: \(m_1 v_1 + m_2 v_2 = 0\)

\(v_2 = -\dfrac{m_1 v_1}{m_2} = -\dfrac{0.020 \times 200}{4} = -1\) m/s.

Answer: Gun recoils at 1 m/s in the direction opposite to the bullet.

v₁ = 200 m/s v₂ = 1 m/s ← Gun (4 kg) Bullet (20 g) Total momentum before = total momentum after = 0
Fig 6.7: Recoil of a gun — bullet and gun acquire equal and opposite momenta.
Activity 6.3 — Balloon RocketL3 Apply
Predict first: A balloon is inflated and released without tying its mouth. Why does it shoot across the room? Which two of Newton's laws does it illustrate?
  1. Inflate a long balloon. Pinch the mouth shut so the air does not escape.
  2. Tape a drinking straw along the upper side of the balloon.
  3. Pass a long thread through the straw and stretch the thread tight across the room.
  4. Release the balloon's mouth and watch it shoot along the thread.
Observation: The balloon zooms forward as the air rushes backward.

Explanation: The balloon pushes air backward (action) and the air pushes the balloon forward (reaction) — Newton's Third Law. Also, the total momentum of (balloon + air) is conserved: the air gains backward momentum, the balloon gains forward momentum so that the sum is zero. This is the same idea behind rockets and jet engines.

More worked numericals

Example 2 — Momentum of a moving body

Q. Find the momentum of a 2 kg ball moving at 3 m/s.

Solution. \(p = mv = 2 \times 3 = 6\) kg·m/s in the direction of motion.

Example 3 — Force from change in momentum

Q. A cricket ball of mass 150 g moving at 20 m/s is brought to rest by a fielder in 0.1 s. Find the force exerted on the ball.

Solution. \(\Delta p = m(v-u) = 0.15(0-20) = -3\) kg·m/s. \(F = \Delta p/t = -3/0.1 = -30\) N. Magnitude of force = 30 N (opposite to motion).

Example 4 — Two-body collision (one body initially at rest)

Q. A truck of mass 2000 kg moving at 5 m/s collides with a stationary car of mass 1000 kg and they move together. Find their common velocity.

Solution. Conservation of momentum: \(m_1 u_1 + m_2 u_2 = (m_1+m_2)v\).

\(2000 \times 5 + 1000 \times 0 = 3000 \times v\) ⇒ \(v = 10000/3000 \approx 3.33\) m/s.

Example 5 — Why bending knees helps

Q. A 60 kg person jumping from a height lands at 4 m/s. Compare the average force on the knees if (i) the person stops in 0.05 s by landing stiff, (ii) stops in 0.5 s by bending the knees.

Solution. \(\Delta p = 60 \times 4 = 240\) kg·m/s.

(i) \(F = 240/0.05 = 4800\) N. (ii) \(F = 240/0.5 = 480\) N.

Bending the knees reduces the force ten-fold by stretching the stopping time — the same lesson behind air-bags and crumple zones.

Example 6 — Two trolleys recoiling

Q. Two boys of mass 40 kg each stand on a frictionless trolley (total mass 100 kg) at rest. One boy jumps off horizontally at 2 m/s. Find the velocity of the trolley + remaining boy.

Solution. Initial momentum = 0. After jump: jumper momentum = 40 × 2 = 80 kg·m/s. Remaining mass = 60 (trolley) + 40 (boy) = 100 kg. So 100 v + 80 = 0 ⇒ v = −0.8 m/s. The trolley moves at 0.8 m/s opposite to the jumper.

Quick Recap

ConceptFormula / Idea
Newton's Third LawForces occur in equal-and-opposite pairs on different bodies.
Momentum\(p = mv\); unit kg·m/s; vector.
2nd Law (momentum form)\(F = \Delta p / t\)
Impulse\(F t = \Delta p\)
Conservation of momentum\(m_1 u_1 + m_2 u_2 = m_1 v_1 + m_2 v_2\) (isolated system)

Competency-Based Questions

In a friendly experiment, two students stand on identical skateboards facing each other on a smooth horizontal floor. Student A (mass 50 kg) throws a 2 kg medicine ball to Student B (mass 40 kg) at 6 m/s relative to the ground.
Q1. With what velocity does Student A move backward after throwing the ball? L3
Initial momentum = 0. After throw: ball = 2 × 6 = 12 kg·m/s forward. Hence A's momentum = −12. \(v_A = -12/50 = -0.24\) m/s. Student A moves backward at 0.24 m/s.
Q2. With what common velocity do Student B and the ball move after B catches it? L3
Before catch: ball momentum = 12, B at rest. After catch: combined mass = 42 kg. \(v = 12/42 \approx 0.286\) m/s in the original direction.
Q3. Which law explains why Student A moves backward? L2
  • (a) Law of inertia
  • (b) Conservation of momentum / Newton's Third Law
  • (c) Newton's Second Law alone
  • (d) Law of friction
(b) The push on the ball is matched by an equal and opposite push on Student A; total momentum stays zero.
Q4. State whether True or False: "When you catch a fast cricket ball you instinctively pull your hands back to reduce the force." L1
True. Pulling the hands back lengthens the stopping time \(t\); since \(F = \Delta p/t\), a larger \(t\) means a smaller force on the hands.
Q5. A 1500 kg car changes its velocity from 10 m/s to 25 m/s in 5 s. Find the magnitude of the force acting on it. L3
\(\Delta p = 1500(25-10) = 22500\) kg·m/s. \(F = 22500/5 = 4500\) N.

Assertion–Reason Questions

Options: (A) Both true, R explains A. (B) Both true, R doesn't explain A. (C) A true, R false. (D) A false, R true.

A: A rocket can move forward in outer space even though there is no air to push against.
R: The rocket exhausts hot gases backward; by Newton's Third Law the gases push the rocket forward.
(A) Both true and R explains A correctly. Rocket motion is a textbook example of the Third Law.
A: The action–reaction forces on a book lying on a table cancel each other out.
R: Action and reaction forces always act on the same body.
(D) Assertion is false (action–reaction forces act on different bodies and so cannot cancel). Reason is also false. Choose (D) only if your option list reads R-true-A-false; here both are false, but standard NCERT answer keys mark such pairs as "Both A and R are false". Final answer: both A and R are false.
A: The total momentum of an isolated system stays constant.
R: An isolated system experiences no net external force.
(A) Both true and R correctly explains A — that is precisely the basis of the conservation law.
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