Q.A batsman deflects a ball by an angle of 45∘ without changing its initial speed which is equal to 54 km/h. What is the impulse imparted to the ball? (Mass of the ball is 0.15 kg.)
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The Intuition: Why Do We Need a "New" Idea?
Imagine you're catching a cricket ball. If you let your hands stay rigid, the ball stings and might bounce off. But if you give with the ball — pulling your hands back as you catch — the catch feels soft and the ball stops gently.
Same ball, same speed, same change in momentum. But the force you feel is completely different. Why?
The answer is time. When you pull your hands back, you increase the time over which the ball slows down. A longer time means a smaller force — even though the total "oomph" needed to stop the ball is the same. That "oomph" is called impulse.
Impulse is not a mysterious new quantity. It's just force multiplied by the time it acts. If you push gently for a long time, or push hard for a short time, you can produce the same effect.
The Precise Statement
The Impulse-Momentum Theorem says:
The impulse delivered to an object equals the change in its momentum.
In symbols:
J=Δp
Where:
- J is the impulse (a vector)
- Δp is the change in momentum (also a vector)
And since impulse is force times time:
FavgΔt=mvf−mvi
J=FavgΔt=Δp
Breaking It Down Piece by Piece
Momentum (p) is mass times velocity: p=mv. It's a measure of how hard it is to stop a moving object. A truck moving slowly has large momentum; a bullet moving fast has large momentum too.
Impulse (J) is the product of the average force and the time interval over which it acts: J=FavgΔt.
The theorem connects them: the net impulse changes the momentum. If you apply a net force to an object for some time, its momentum changes by exactly that amount.
A common mistake is to think impulse is just force. It's force × time. A huge force acting for a tiny time (like a bat hitting a ball) can produce the same impulse as a tiny force acting for a long time (like a gentle push).
Why This Matters: Real-World Examples
Catching a ball (soft vs. hard hands)
- Hard hands: Δt is small → Favg is large (it hurts)
- Soft hands: Δt is large → Favg is small (it's comfortable)
- In both cases, Δp is the same (ball goes from moving to stopped)
Airbags in cars
- Without airbag: your head hits the dashboard in ~0.01 s → huge force
- With airbag: your head decelerates over ~0.1 s → force is 10 times smaller
- Same change in momentum, but the airbag extends the time
A cricket bat hitting a ball
- The bat is in contact with the ball for a few milliseconds
- The force during that contact is enormous (hundreds of Newtons)
- The impulse changes the ball's momentum from one direction to another
The Mathematical Derivation (Short)
Start from Newton's second law:
Fnet=ma=mdtdv
Multiply both sides by dt:
Fnetdt=mdv
Integrate over the time interval:
∫titfFnetdt=m∫vivfdv=mvf−mvi
The left side is the impulse (the area under the force-time graph). The right side is the change in momentum. …
Impulse-Momentum Theorem: J=Δp=m(vf−vi).
Step 1: Convert speed to SI units: 54 km/h =54×185=15 m/s.
Step 2: The initial and final velocity vectors have equal magnitude v=15 m/s, separated by 45∘ (deflection, speed unchanged). For two equal-magnitude vectors with angle θ between them:
∣Δv∣=2vsin(2θ)
Step 3: With θ=45∘:
∣Δv∣=2(15)sin(22.5∘)≈2(15)(0.3827)≈11.48 m/s
Step 4: Impulse magnitude: …
Impulse equals the change in momentum. The speed is unchanged, so only the direction changes by 45∘; treating the initial and final velocity vectors as two equal-magnitude sides of an isosceles triangle gives ∣Δv∣=2vsin(θ/2). With v=15 m s−1 and θ=45∘: J≈1.72 N⋅s.
Concept
By the impulse–momentum theorem, J=Δp=mvf−mvi. Even though the speed is unchanged, momentum is a vector, so a change of direction gives a non-zero impulse. The initial velocity vi and final velocity vf have the same magnitude v, with the angle between them equal to the 45∘ deflection. Geometrically, vi, vf, and Δv=vf−vi form an isosceles triangle with two sides of length v and included angle θ.
Step 1 — Convert the speed
v=54 km/h=54×185=15 m s−1
Step 2 — Magnitude of the velocity change
For an isosceles triangle with two sides v and included angle θ, the base (the magnitude of Δv) is:
∣Δv∣=v2+v2−2v2cosθ=v2(1−cosθ)=2vsin(2θ)
With θ=45∘:
∣Δv∣=2(15)sin(22.5∘)=30×0.3827≈11.48 m s−1 …
Concept: Impulse as a Vector Change in Momentum (Speed Unchanged, Direction Changed)
Step 1: Convert the speed to SI units
v=54 km/h=54×185=15 m s−1
Step 2: Set up the geometry of Δv
vi and vf have equal magnitude v with the angle between them equal to
the deflection θ=45∘. They form two equal sides of an isosceles triangle
with included angle θ; the third side is ∣Δv∣:
∣Δv∣=v2+v2−2v2cosθ=2vsin(2θ)
Step 3: Compute the magnitude of Δv
∣Δv∣=2(15)sin(22.5∘)≈30×0.3827≈11.48 m s−1 …
- KEAM 2026Set eng-2026-04184 marksMCQQ.A batsman hits a cricket ball of mass 0.15 kg travelling at a speed of 54 kmph. The ball reverses its direction. The impulse imparted to the ball in kgms−1 is (A) 4.5 (B) 45 (C) 810 (D) 8.1 (E) 16.2
›Reveal solutionSolution
The ball reverses, so the change in momentum is 2mv; with v=54 kmph=15 m/s this gives 4.5 kg m/s.
Convert 54 kmph=54×185=15 m/s. Reversal changes the velocity from +v to −v, so …
- KEAM 2026Set eng-2026-04194 marksMCQQ.A ball of 200 g mass moving with a speed of 5 ms−1 collides with a wall and bounces back with the same speed. If the force exerted on the wall is 1 N, then the ball is in contact with the wall for (A) 2 s (B) 1 s (C) 0.5 s (D) 1.5 s (E) 0.75 s
›Reveal solutionSolution
The change in momentum on rebound is 2mv; contact time =Δp/F.
The ball reverses direction with the same speed, so the change in momentum has magnitude
Δp=mv−(−mv)=2mv=2(0.2 kg)(5 m s−1)=2 kg m s−1. …
- KEAM 2026Set eng-2026-04224 marksMCQQ.If the area under the graph between the force on an object and time is 20 units, then the object experiences (A) an impulse of 10 units (B) a change of momentum of 10 units (C) an impulse of 20 units (D) a change of force by 20 units (E) a change of acceleration of 20 units
›Reveal solutionSolution
The area under a force–time graph equals impulse (and hence the change in momentum), numerically 20.
Impulse J=∫Fdt= area under the F–t graph =20 units. …
- KEAM 2026Set pha-2026-0420F4 marksMCQQ.0.2 kg ball strikes a wall with velocity 10 ms−1 and rebounds with 8 ms−1. The impulse delivered by the ball is (A) 0.4 Ns (B) 3.6 Ns (C) 1.4 Ns (D) 1.8 Ns (E) 16.0 Ns
›Reveal solutionSolution
Taking rebound velocity as opposite in sign, Δp=m(v2−v1)=0.2(18)=3.6 Ns.
Impulse equals the change in momentum. Take the incoming direction as positive: v1=+10m/s, and after rebound the ball moves the other way, v2=−8m/s. …
- KEAM 2025Set eng-2025-04254 marksMCQQ.If a ball of mass 0.02 kg bowled by a bowler straight to a batsman is hit back with the same speed with an impulse of 2 Ns, then the speed of the ball bowled is (A) 20 ms−1 (B) 80 ms−1 (C) 50 ms−1 (D) 60 ms−1 (E) 40 ms−1
›Reveal solutionSolution
The ball reverses direction with equal speed, so the impulse equals 2mv. Solving 2=2(0.02)v gives v=50 m s−1.
Take the incoming direction as positive. The ball arrives with velocity +v and leaves with velocity −v (same speed, reversed).
Impulse = change in momentum:
J=mvf−mvi=m(−v)−m(v)=−2mv.
The magnitude is
J=2mv. …
- KEAM 2025Set eng-2025-04274 marksMCQQ.A tennis ball of mass 150 g is moving at 20 ms−1. A racket strikes it, reversing its direction with a final speed of 30 ms−1. If the contact time is 0.02 s, then the magnitude of the force (in N) exerted by the racket is (A) 1.5 N (B) 3.75 N (C) 15 N (D) 150 N (E) 375 N
›Reveal solutionSolution
The ball reverses direction, so the speed change in magnitude is 20+30=50 m/s. F=ΔtmΔv=0.020.15×50=375 N.
Take the initial direction as positive: vi=+20 m/s, and after the strike the ball moves the opposite way at 30 m/s, so vf=−30 m/s. The change in momentum is
Δp=m(vf−vi)=0.15(−30−20)=−7.5 kg m s−1, …
- KEAM 2025Set eng-2025-04284 marksMCQQ.A body of mass 5 kg collides with a wall with a speed of 50 ms−1 and rebounds with the same speed. If the time of contact of the body with the wall is 201s the force exerted on the wall is (A) 0.5×104N (B) 2.5×104N (C) 2×103N (D) 1×104N (E) 4×103N
›Reveal solutionSolution
On rebounding with equal speed, Δp=m(2v)=500; F=Δp/Δt=500×20=1×104 N.
The body rebounds with the same speed in the opposite direction, so the magnitude of the change in momentum is
Δp=m∣vf−vi∣=5×∣50−(−50)∣=5×100=500 kgms−1.
The average force is …
- KEAM 2025Set pha-2025-0424A4 marksMCQQ.The area under the curve drawn between the force F and time t is (A) torque (B) impulse (C) work done (D) power (E) kinetic energy
›Reveal solutionSolution
Impulse J=∫Fdt, which is exactly the area under the F vs t curve, and equals the change in momentum. …
- KEAM 2025Set pha-2025-0429F4 marksMCQQ.A hockey player hits a ball with an impulse of 15 Ns. If time of hit is 0.2 s, the average force exerted by the player on the ball is (A) 75 N (B) 50 N (C) 15 N (D) 20 N (E) 25 N
›Reveal solutionSolution
Impulse equals average force times contact time, so Favg=J/t=15/0.2=75N.
Impulse is defined as J=FavgΔt. Rearranging for the average force: …
- KEAM 2024Set eng-2024-06064 marksMCQQ.When a cricketer catches a ball in 30 s, the force required is 2.5 N. The force required to catch that ball in 50 s is (A) 1.5 N (B) 1 N (C) 2.5 N (D) 3 N (E) 5 N
›Reveal solutionSolution
Same momentum change over a longer time means a smaller force: F=Δp/t gives 1.5 N.
The ball's momentum change Δp is the same in both cases, and F=tΔp, so F∝t1. Therefore …
- KEAM 2021Set eng-2021-P1-A14 marksMCQQ.Area under the force-time graph gives the change in (A) velocity (B) acceleration (C) linear momentum (D) angular momentum (E) impulsive force
›Reveal solutionSolution
Area under the force-time graph equals the change in linear momentum.
Concept and Intuition
Impulse is defined as J=∫Fdt, the area under the force-time curve. The impulse-momentum theorem states this impulse equals the change in linear momentum Δp.
Step-by-Step Solution
- J=∫Fdt= area under the F-t graph.
- F=dtdp⇒∫Fdt=Δp. …
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