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JEE Advanced 2024 · Motion in a Plane

A ball is thrown from the location (x0,y0)=(0,0)(x_0, y_0) = (0,0) of a horizontal playground with an initial speed v0v_0 at an angle θ0\theta_0 from the +x+x-direction. The ball is to be hit by a stone, which is thrown at the same time from the location (x1,y1)=(l,0)(x_1, y_1) = (l, 0). The stone is thrown at an angle (180−θ1)(180 - \theta_1) from the +x+x-direction with a suitable initial speed. For a fixed v0v_0, when (θ0,θ1)=(45∘,45∘)(\theta_0, \theta_1) = (45^\circ, 45^\circ), the stone hits the ball after time T1T_1, and when (θ0,θ1)=(60∘,30∘)(\theta_0, \theta_1) = (60^\circ, 30^\circ), it hits the ball after time T2T_2. In such a case, (T1T2)2\left(\frac{T_1}{T_2}\right)^2 is ______.

Answer: 22

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Written solution

Step 1: Analyze the vertical motion.

For the ball and the stone to collide, their vertical coordinates must be equal at the time of collision.

yb(t)=v0sin⁡θ0 t−12gt2y_b(t) = v_0\sin\theta_0\, t - \frac{1}{2} g t^2 ys(t)=usin⁡θ1 t−12gt2y_s(t) = u\sin\theta_1\, t - \frac{1}{2} g t^2

Equating yb(t)=ys(t)y_b(t) = y_s(t) yields the relation between their initial vertical velocities.

v0sin⁡θ0=usin⁡θ1v_0\sin\theta_0 = u\sin\theta_1

Step 2: Analyze the horizontal motion.

The sum of the horizontal distances covered by both objects at the time of collision TT must equal the initial separation ll.

l=(v0cos⁡θ0+ucos⁡θ1) Tl = (v_0\cos\theta_0 + u\cos\theta_1)\, T

Step 3: Express the collision time TT.

Solve for uu from the vertical motion relation and substitute it into the horizontal motion equation.

u=v0sin⁡θ0sin⁡θ1u = \frac{v_0\sin\theta_0}{\sin\theta_1} l=T(v0cos⁡θ0+v0sin⁡θ0cos⁡θ1sin⁡θ1)l = T\left(v_0\cos\theta_0 + \frac{v_0\sin\theta_0\cos\theta_1}{\sin\theta_1}\right)

Simplify using the angle addition formula for sine.

l=Tv0(sin⁡θ1cos⁡θ0+sin⁡θ0cos⁡θ1sin⁡θ1)l = T v_0 \left(\frac{\sin\theta_1\cos\theta_0 + \sin\theta_0\cos\theta_1}{\sin\theta_1}\right) l=Tv0sin⁡(θ0+θ1)sin⁡θ1l = T v_0 \frac{\sin(\theta_0 + \theta_1)}{\sin\theta_1} T=lsin⁡θ1v0sin⁡(θ0+θ1)T = \frac{l\sin\theta_1}{v_0\sin(\theta_0 + \theta_1)}

Step 4: Calculate the collision times T1T_1 and T2T_2.

For Case 1, (θ0,θ1)=(45∘,45∘)(\theta_0, \theta_1) = (45^\circ, 45^\circ), which gives θ0+θ1=90∘\theta_0 + \theta_1 = 90^\circ.

T1=lsin⁡45∘v0sin⁡90∘=l2v0T_1 = \frac{l\sin 45^\circ}{v_0\sin 90^\circ} = \frac{l}{\sqrt{2}v_0}

For Case 2, (θ0,θ1)=(60∘,30∘)(\theta_0, \theta_1) = (60^\circ, 30^\circ), which also gives θ0+θ1=90∘\theta_0 + \theta_1 = 90^\circ.

T2=lsin⁡30∘v0sin⁡90∘=l2v0T_2 = \frac{l\sin 30^\circ}{v_0\sin 90^\circ} = \frac{l}{2v_0}

Step 5: Find the ratio of the squared times.

Divide T1T_1 by T2T_2 and square the result.

T1T2=l2v0l2v0=2\frac{T_1}{T_2} = \frac{\frac{l}{\sqrt{2}v_0}}{\frac{l}{2v_0}} = \sqrt{2} (T1T2)2=2\left(\frac{T_1}{T_2}\right)^2 = 2

Answer: 2

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