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JEE Advanced 2002 · Motion in a Straight Line

On a frictionless horizontal surface, assumed to be the xx-yy plane, a small trolley AA is moving along a straight line parallel to the yy-axis (see figure) with a constant velocity of (3−1) m/s(\sqrt{3}-1)\,\text{m/s}. At a particular instant, when the line OAOA makes an angle of 45∘45^\circ with the xx-axis, a ball is thrown along the surface from the origin OO. Its velocity makes an angle ϕ\phi with the xx-axis and it hits the trolley. (a) The motion of the ball is observed from the frame of the trolley. Calculate the angle θ\theta made by the velocity vector of the ball with the xx-axis in this frame. (b) Find the speed of the ball with respect to the surface, if ϕ=40/3\phi = 40/3.

Answer: 45°,2m/s45°,2 m/s

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Written solution

Step 1: Define the coordinates and initial positions.

Let the origin O(0,0)O(0,0) be the projection point of the ball, and let the trolley AA move along the line x=ax = a.

r⃗A(0)=(a,a)\vec{r}_A(0) = (a, a)

Step 2: Write the position vectors as functions of time.

The trolley moves parallel to the yy-axis with constant velocity vA=3−1v_A = \sqrt{3}-1.

r⃗A(t)=(a,a+vAt)\vec{r}_A(t) = (a, a + v_A t)

The ball is projected from the origin with speed uu at an angle ϕ\phi with the xx-axis.

r⃗ball(t)=(ucos⁡ϕ t,usin⁡ϕ t)\vec{r}_{\text{ball}}(t) = (u\cos\phi\,t, u\sin\phi\,t)

Step 3: Apply the condition for the ball to hit the trolley.

At the instant of collision tt, the position vectors of the ball and the trolley must be equal.

ucos⁡ϕ t=au\cos\phi\,t = a usin⁡ϕ t=a+vAtu\sin\phi\,t = a + v_A t

Substitute the first equation into the second equation.

usin⁡ϕ t=ucos⁡ϕ t+vAtu\sin\phi\,t = u\cos\phi\,t + v_A t

Divide both sides by tt.

usin⁡ϕ−ucos⁡ϕ=vAu\sin\phi - u\cos\phi = v_A

Step 4: Determine the relative velocity and the angle θ\theta in the trolley's frame.

The velocity of the ball relative to the trolley is the difference of their velocities.

v⃗rel=v⃗ball−v⃗A\vec{v}_{\text{rel}} = \vec{v}_{\text{ball}} - \vec{v}_A v⃗rel=(ucos⁡ϕ,usin⁡ϕ−vA)\vec{v}_{\text{rel}} = (u\cos\phi, u\sin\phi - v_A)

Substitute usin⁡ϕ−vA=ucos⁡ϕu\sin\phi - v_A = u\cos\phi into the relative velocity vector.

v⃗rel=(ucos⁡ϕ,ucos⁡ϕ)\vec{v}_{\text{rel}} = (u\cos\phi, u\cos\phi)

Calculate the angle θ\theta of this relative velocity vector with the xx-axis.

tan⁡θ=ucos⁡ϕucos⁡ϕ=1\tan\theta = \frac{u\cos\phi}{u\cos\phi} = 1 θ=45∘\theta = 45^\circ

Step 5: Calculate the speed of the ball with respect to the surface.

The given angle satisfies tan⁡ϕ=4/3\tan\phi = 4/3.

sin⁡ϕ=45\sin\phi = \frac{4}{5} cos⁡ϕ=35\cos\phi = \frac{3}{5}

Substitute these values into the collision relation.

u(45−35)=vAu\left(\frac{4}{5} - \frac{3}{5}\right) = v_A u5=3−1\frac{u}{5} = \sqrt{3}-1 u=5(3−1) m/su = 5(\sqrt{3}-1)\,\text{m/s} u≈3.66 m/su \approx 3.66\,\text{m/s}

Answer: (a) θ=45∘\theta = 45^\circ (b) u=5(3−1) m/s≈3.66 m/su = 5(\sqrt{3}-1)\,\text{m/s} \approx 3.66\,\text{m/s}

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