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Calculate Train Acceleration to Catch Thrown Ball

A train is moving along a straight line with a constant acceleration 'aa'. A boy standing in the train throws a ball forward with a speed of 10 m/s10\text{ m/s}, at an angle of 60∘60^\circ to the horizontal. The boy has to move forward by 1.15 m1.15\text{ m} inside the train to catch the ball back at the initial height. The acceleration of the train, in m/s2\text{m/s}^2, is

Official Numerical Answer5

Step-by-Step Solution

To find the acceleration of the train, we analyze the motion of the ball in the non-inertial frame of reference of the train.

1. Motion relative to the Train

Let the train be accelerating in the horizontal xx-direction with a constant acceleration aa. In the frame of reference of the train, the pseudo-acceleration acting on the ball is −ai^-a\hat{i}, and the acceleration due to gravity is −gj^-g\hat{j} (where g=10 m/s2g = 10\text{ m/s}^2).

  • Initial velocity of the ball relative to the train:
    ux,rel=ucos⁡60∘=10×12=5 m/su_{x, \text{rel}} = u \cos 60^\circ = 10 \times \frac{1}{2} = 5\text{ m/s}
    uy,rel=usin⁡60∘=10×32=53 m/su_{y, \text{rel}} = u \sin 60^\circ = 10 \times \frac{\sqrt{3}}{2} = 5\sqrt{3}\text{ m/s}

  • Accelerations relative to the train:
    ax,rel=−aa_{x, \text{rel}} = -a
    ay,rel=−g=−10 m/s2a_{y, \text{rel}} = -g = -10\text{ m/s}^2


2. Time of Flight

The ball returns to its initial vertical height when its vertical displacement relative to the train becomes zero:
yrel=uy,relT−12gT2=0y_{\text{rel}} = u_{y, \text{rel}} T - \frac{1}{2} g T^2 = 0

Solving for the time of flight TT (for T≠0T \neq 0):
T=2uy,relg=2×5310=3 sT = \frac{2 u_{y, \text{rel}}}{g} = \frac{2 \times 5\sqrt{3}}{10} = \sqrt{3}\text{ s}

Thus, T2=3 s2T^2 = 3\text{ s}^2.


3. Horizontal Displacement inside the Train

The boy has to move forward by 1.15 m1.15\text{ m} inside the train to catch the ball. Therefore, the horizontal displacement of the ball relative to the train during the time of flight TT is xrel=1.15 mx_{\text{rel}} = 1.15\text{ m}.

Using the kinematic equation for horizontal motion relative to the train:
xrel=ux,relT+12ax,relT2x_{\text{rel}} = u_{x, \text{rel}} T + \frac{1}{2} a_{x, \text{rel}} T^2

Substitute the known values into the equation:
1.15=5T−12aT21.15 = 5 T - \frac{1}{2} a T^2

Substitute T=3 sT = \sqrt{3}\text{ s} and T2=3T^2 = 3:
1.15=53−32a1.15 = 5\sqrt{3} - \frac{3}{2} a

Taking 3≈1.732\sqrt{3} \approx 1.732:
1.15≈5(1.732)−1.5a1.15 \approx 5(1.732) - 1.5 a
1.15≈8.66−1.5a1.15 \approx 8.66 - 1.5 a

Rearranging to solve for aa:
1.5a=8.66−1.151.5 a = 8.66 - 1.15
1.5a=7.51≈7.51.5 a = 7.51 \approx 7.5
a=7.51.5=5 m/s2a = \frac{7.5}{1.5} = 5\text{ m/s}^2

Thus, the acceleration of the train is 5 m/s25\text{ m/s}^2.