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Question: A particle strikes a horizontal frictionless floor with a speed \( u \) at angle \( \theta \) with t...

A particle strikes a horizontal frictionless floor with a speed uu at angle θ\theta with the vertical, and rebounds with a speed vv at angle ϕ\phi with the vertical. The coefficient of restitution between the particle and floor is ee . The magnitude of vv is

A. eueu
B. (1e)u\left( {1 - e} \right)u
C. ue2sin2θ+cos2θu\sqrt {{e^2}{{\sin }^2}\theta + {{\cos }^2}\theta }
D. usin2θ+e2cos2θu\sqrt {{{\sin }^2}\theta + {e^2}{{\cos }^2}\theta }

Explanation

Solution

In this given question, we have to use the concept of conservation of momentum to formulate the first equation. Then by applying the formula of the coefficient of restitution we will find another equation. Hence, by solving the two formulas we will find the answer.

Complete answer:
In the given question it is mentioned that the floor is frictionless. The initial velocity of the particle when it strikes the floor is uu and the angle at which it strikes the floor is θ\theta in the vertical direction.
The particle again rebounds with the final velocity vv at angle ϕ\phi in the vertical direction.
From the momentum of conservation we get,
musinθ=mvsinϕmu\sin \theta = mv\sin \phi
By arranging the equation and dividing it by mm we get,
Or, vsinϕ=usinθ(1)v\sin \phi = u\sin \theta - - - - - \left( 1 \right)
Again, from the coefficient of restitution ee in the vertical direction, we get,
vcosϕucosθ=e\dfrac{{v\cos \phi }}{{u\cos \theta }} = e
Or, vcosϕ=eucosθ(2)v\cos \phi = eu\cos \theta - - - - - \left( 2 \right)
Now, by squaring and adding equation (1)\left( 1 \right) and equation (2)\left( 2 \right) we get,
v2sin2ϕ+v2cos2ϕ=u2sin2θ+e2u2cos2θ{v^2}{\sin ^2}\phi + {v^2}{\cos ^2}\phi = {u^2}{\sin ^2}\theta + {e^2}{u^2}{\cos ^2}\theta
Taking v2{v^2} common in the left hand side and u2{u^2} from the right hand side of the equation, we get,
v2(sin2θ+cos2θ)=u2(sin2θ+e2cos2θ){v^2}\left( {{{\sin }^2}\theta + {{\cos }^2}\theta } \right) = {u^2}\left( {{{\sin }^2}\theta + {e^2}{{\cos }^2}\theta } \right)
From trigonometric identity we know that, sin2θ+cos2θ=1{\sin ^2}\theta + {\cos ^2}\theta = 1
Substituting its value we get,
v2=u2(sin2θ+e2cos2θ){v^2} = {u^2}\left( {{{\sin }^2}\theta + {e^2}{{\cos }^2}\theta } \right)
From the square root of both sides we get,
v=u2(sin2θ+e2cos2θ)=u(sin2θ+e2cos2θ)v = \sqrt {{u^2}\left( {{{\sin }^2}\theta + {e^2}{{\cos }^2}\theta } \right)} = u\sqrt {\left( {{{\sin }^2}\theta + {e^2}{{\cos }^2}\theta } \right)}
So, the magnitude of vv is u(sin2θ+e2cos2θ)u\sqrt {\left( {{{\sin }^2}\theta + {e^2}{{\cos }^2}\theta } \right)} .
The correct option is D. usin2θ+e2cos2θu\sqrt {{{\sin }^2}\theta + {e^2}{{\cos }^2}\theta } .

Note:
It must be noted that we have formulated the equation of momentum conservation using sine angle as the question provided information about the vertical component only. The coefficient of restitution is the ratio of the final relative speed to the initial relative speed between two objects after their collision.