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Question: A small ball is projected up a smooth inclined plane with an initial speed of \(10\,m{\text{ }}{s^{ ...

A small ball is projected up a smooth inclined plane with an initial speed of 10m s110\,m{\text{ }}{s^{ - 1}} along the direction at 30{30^ \circ } to the bottom edge of the slope. It returns to the edge after 2s2\,s . The ball is in contact with the inclined plane throughout the process. What is the inclination angle of the plane?

Explanation

Solution

To solve this question, one must know about motion in projectile, here we have redrawn the figure which is given above after that applying equation of motion in the y-axis we have solved for the required data i.e., inclination angle of the plane or the same question is done with the help of the formula of time of flight.

Formula used:
s=ut+12at2s = ut + \dfrac{1}{2}a{t^2}
t=2usinθgt = \dfrac{{2u\sin \theta }}{g}
Where, ss is the distance, uu is the initial velocity, tt is the time, aa is acceleration and
gg is the acceleration due to gravity.

Complete step by step answer:

According to the question, the initial speed of the ball is 10m s110\,m{\text{ }}{s^{ - 1}}.Angle with the ball on the slope is, 30{30^ \circ }. The net acceleration towards the bottom is, gsinθg\sin \theta . And assuming acceleration due to gravity along the slope is, 10m s210\,m{\text{ }}{s^{ - 2}}.

We can say that in the direction motion the final displacement is zero because from where the ball starts comes to the same position in the y-axis. So, using equation of motion, along y-axis,
Sy=uy+t+12ayt2{S_y} = {u_y} + t + \dfrac{1}{2}{a_y}{t^2}
Sy=0\Rightarrow {S_y} = 0
t=2s\Rightarrow t = 2s
uy=10sin30=5m s1\Rightarrow {u_y} = 10\sin {30^ \circ } = 5m{\text{ }}{s^{ - 1}}
And a=gsinθa = g\sin \theta
So,
0=5×212×10sinθ×4 2sinθ=1 sinθ=12 0 = 5 \times 2 - \dfrac{1}{2} \times 10\sin \theta \times 4 \\\ \Rightarrow 2\sin \theta = 1 \\\ \Rightarrow \sin \theta = \dfrac{1}{2} \\\
θ=30\therefore \theta = {30^ \circ }

Hence, 30{30^ \circ } is the inclination angle of the plane.

Note: Note that we can easily done same question, by using the formula of time of flight i.e., T=2usinθgT = \dfrac{{2u\sin \theta }}{g}
As the time of flight is given i.e., T=2sT = 2s
g=gsinθg = g\sin \theta
And u=10m s1u = 10m{\text{ }}{s^{ - 1}}
so simply putting the value and solving for θ\theta .
2=2×10sin30gsinθ2 = \dfrac{{2 \times 10\sin {{30}^ \circ }}}{{g\sin \theta }}
2=2×10sin30gsinθ sinθ=12 θ=30 \Rightarrow 2 = \dfrac{{2 \times 10\sin {{30}^ \circ }}}{{g\sin \theta }} \\\ \Rightarrow \sin \theta = \dfrac{1}{2} \\\ \therefore \theta = {30^ \circ } \\\
The motion of an item hurled or projected into the air, subject only to gravity's acceleration, is known as projectile motion. The object is known as a projectile, and the course it takes is known as a trajectory. Falling object motion is a simple one-dimensional type of projectile motion with no horizontal movement, as described in Problem-Solving Basics for One-Dimensional Kinematics.