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Question: A ball thrown from position A against a smooth circular wall rebounds and hits position B at the oth...

A ball thrown from position A against a smooth circular wall rebounds and hits position B at the other end of the diameter through A. If the coefficient of restitution between wall and ball is ee and θ=30\theta = {30^ \circ } , then find 3e3e . Do not consider any force on the ball except contact force due to the wall at the time of the collision.
(A) 11
(B) 14\dfrac{1}{4}
(C) 15\dfrac{1}{5}
(D) 3\sqrt 3

Explanation

Solution

It is known that the coefficient of restitution is defined as the ratio of the final to initial relative velocity between two objects after they collide. Expression for the coefficient of restitution for a body colliding with an rigid body at rest is given by, e=vnormalunormale = \dfrac{{{v_{normal}}}}{{{u_{normal}}}} where, vnormal{v_{normal}} is the component of the final velocity normal with the impact surface and unormal{u_{normal}} is the component of the initial velocity normal with the impact surface.

Complete step by step solution:
We know that the coefficient of restitution is defined as the ratio of the final to initial relative velocity between two objects after they collide.
Expression for the coefficient of restitution for a body colliding with an rigid body at rest is given by, e=vnormalunormale = \dfrac{{{v_{normal}}}}{{{u_{normal}}}} where, vnormal{v_{normal}} is the component of the final velocity normal with the impact surface and unormal{u_{normal}} is the component of the initial velocity normal with the impact surface.
Now, here we have a circular wall as an impact surface. So, the normal component of velocity will be along the normal of the circle.
Now, let's say the initial velocity of the ball is uu and final velocity of the ball is vv .
From the figure we can see that the normal component (along ODOD ) of initial velocity is the same as the horizontal component of the initial velocity (along ABAB ), since the ΔAOB\Delta AOB is an isosceles triangle. So, we can take the normal (along ODOD ) and tangential(along the tangent of the circle) component of velocity as mutually orthogonal components as in the polar coordinate system.

So, we can write, unormal=ucosθ{u_{normal}} = u\cos \theta and utangential=usinθ{u_{tangential}} = u\sin \theta
For, final velocity vnormal=vsinθ{v_{normal}} = v\sin \theta and vtangential=vcosθ{v_{tangential}} = v\cos \theta .
So, the coefficient of restitution becomes, e=vnormalunormal=vsinθucosθe = \dfrac{{{v_{normal}}}}{{{u_{normal}}}} = \dfrac{{ - v\sin \theta }}{{u\cos \theta }} [ Since, they are in opposite direction.]
Simplifying we get, eucosθ=vsinθeu\cos \theta = - v\sin \theta
Since, we know the horizontal component of the velocity does not change due to collision so we can write, utangential=vtangential{u_{tangential}} = {v_{tangential}}
Or, usinθ=vcosθu\sin \theta = v\cos \theta .
taking only magnitude and rewriting the equations we get,
eucosθ=vsinθeu\cos \theta = v\sin \theta
and, usinθ=vcosθu\sin \theta = v\cos \theta .
Dividing the equations we get,
ecotθ=tanθe\cot \theta = \tan \theta
Or, e=tan2θe = {\tan ^2}\theta
Here, given θ=30\theta = {30^ \circ } . Putting the value we get,
e=(13)2=13e = {\left( {\dfrac{1}{{\sqrt 3 }}} \right)^2} = \dfrac{1}{3}
Or, 3e=13e = 1
Hence, the magnitude of 3e3e is 11. So, option (A ) is correct.

Note:
\bullet The tangential component of the velocity is always acting tangentially though the magnitude of the initial and final velocity is different along the tangential direction in the Cartesian system but they are always equivalent in the polar coordinate system. If the collision happened with a smooth perpendicular wall then one has to use the components in the Cartesian coordinate system.
\bullet Collision of an object with body at rest is always two dimensional