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Question: A boy is standing on a cart moving along the\[x - \] axis with a speed of \[10\,{\text{m}}{{\text{s}...

A boy is standing on a cart moving along thexx - axis with a speed of 10ms110\,{\text{m}}{{\text{s}}^{ - 1}} . When the cart reaches the origin, he throws a stone in the horizontal xyx - y plane, with a speed of 5ms15\,{\text{m}}{{\text{s}}^{ - 1}} with respect to himself at an angle θ\theta with the xx - axis. It is found that the stone hits a ball lying at rest at a point whose coordinates are (3m,1m)\left( {\sqrt 3 \,{\text{m}},\,1\,{\text{m}}} \right) . The value of θ\theta is (gravitational effects are to be ignored).
(A) 3030^\circ
(B) 6060^\circ
(C) 9090^\circ
(D) 120120^\circ

Explanation

Solution

First of all, we will find the horizontal and vertical components of the velocity of the ball. Then we will find out the expression for vertical and horizontal distances using the components of velocities and the coordinate point given. We will manipulate the two expressions accordingly and obtain the result.

Complete step by step answer:
In the given question, we are supplied the following data:
The velocity of the boy is 10ms110\,{\text{m}}{{\text{s}}^{ - 1}} who is moving along the xx - axis.
The velocity with which he throws the ball is 5ms15\,{\text{m}}{{\text{s}}^{ - 1}} .
The boy throws the ball at an angle θ\theta with the xx - axis.
The stone hits a ball which is at rest at a point with coordinates (3m,1m)\left( {\sqrt 3 \,{\text{m}},\,1\,{\text{m}}} \right) .
We are asked to find the angle with the xx - axis at which the stone was thrown.
To have a better understanding, we draw a simple diagram, as below:

First, we will find the two components of the velocity of the stone.
Since, the velocity of the stone contains the velocity at which it was thrown and the velocity of the boy as well.
The horizontal component of the velocity is:
vx=(10+5cosθ)ms1\Rightarrow{v_{\text{x}}} = \left( {10 + 5\cos \theta } \right)\,{\text{m}}{{\text{s}}^{ - 1}}
The vertical component of the velocity is:
vy=5sinθ\Rightarrow{v_{\text{y}}} = 5\sin \theta
The point at which the ball is (3m,1m)\left( {\sqrt 3 \,{\text{m}},\,1\,{\text{m}}} \right) .
So, the horizontal distance is 3m\sqrt 3 \,{\text{m}} and the vertical distance is 1m1\,{\text{m}} .
By applying the formula which relates velocity, distance and time is:
distance=velocity×time\Rightarrow{\text{distance}} = {\text{velocity}} \times {\text{time}}……(1)
By substituting the required values (for the horizontal and vertical) in the equation (1), we get:
3=(10+5cosθ)t\Rightarrow\sqrt 3 = \left( {10 + 5\cos \theta } \right)t …… (2)
1=(5sinθ)×t\Rightarrow 1 = \left( {5\sin \theta } \right) \times t …… (3)
Now, we divide the equation (2) by equation (3), and we get:
31=10+5cosθ5sinθ 53sinθ=10+5cosθ 3sinθ=2+cosθ 3sinθcosθ=2  \Rightarrow\dfrac{{\sqrt 3 }}{1} = \dfrac{{10 + 5\cos \theta }}{{5\sin \theta }} \\\ \Rightarrow 5\sqrt 3 \sin \theta = 10 + 5\cos \theta \\\ \Rightarrow\sqrt 3 \sin \theta = 2 + \cos \theta \\\ \Rightarrow\sqrt 3 \sin \theta - \cos \theta = 2 \\\
Now, we divide the two sides by a factor 22
32sinθ12cosθ=1 sinθcos(π6)sin(π6)cosθ=1 sin(θπ6)=sinπ2 θπ6=π2  \Rightarrow\dfrac{{\sqrt 3 }}{2}\sin \theta - \dfrac{1}{2}\cos \theta = 1 \\\ \Rightarrow\sin \theta \cos \left( {\dfrac{\pi }{6}} \right) - \sin \left( {\dfrac{\pi }{6}} \right)\cos \theta = 1 \\\ \Rightarrow \sin \left( {\theta - \dfrac{\pi }{6}} \right) = \sin \dfrac{\pi }{2} \\\ \Rightarrow \theta - \dfrac{\pi }{6} = \dfrac{\pi }{2} \\\
Simplifying again we get:

θ=π2+π6 θ=3π+π6 θ=4π6 θ=2π3 θ=120\Rightarrow\theta = \dfrac{\pi }{2} + \dfrac{\pi }{6} \\\ \Rightarrow\theta = \dfrac{{3\pi + \pi }}{6} \\\ \Rightarrow\theta = \dfrac{{4\pi }}{6} \\\ \Rightarrow\theta = \dfrac{{2\pi }}{3} \\\ \Rightarrow\theta = 120^\circ

Hence, the value of θ\theta is 120120^\circ .

The correct option is D.

Note: It is important to note that many students tend to make mistakes while finding the horizontal component of velocity. They just write 5cosθ5\cos \theta which is wrong, as the boy was also in motion while throwing the ball. His velocity must also be taken into account.