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Karnataka Board PUCPUC Science Class 11

A Projectile is Fired with a Speed U at an Angle θ Above a Horizontal Field. the Coefficient of Restitution of Collision Between the Projectile and the Field is E. How Far from the Starting Point - Physics

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Question

A projectile is fired with a speed u at an angle θ above a horizontal field. The coefficient of restitution of collision between the projectile and the field is e. How far from the starting point, does the projectile makes its second collision with the field? 

Numerical
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Solution

Given:
Initial velocity of the projectile = u
Angle of projection of the projectile with respect to ground = θ

When the projectile hits the ground for the first time, the velocity remains same i.e. u.
The component of velocity parallel to ground, u cos θ should remain constant.
However, the vertical component of the projectile undergoes a change after the collision. 


If the coefficient of restitution of collision between the projectile and the field is e,
The velocity of separation is given by, 
⇒ v = eu sin θ

Therefore, for the second projectile motion,
Velocity of projection (u') will be,

\[u' = \sqrt{(u \cos \theta )^2 + (eu \sin \theta )^2}\]

\[\text{ Angle of projection,} \alpha = \tan^{- 1} \left( \frac{eu \sin \theta}{u \cos \theta} \right)\]

\[ \Rightarrow \alpha = \tan^{- 1} (e \tan \theta)\]

\[\text{or}, \tan \alpha = e \tan \theta . . . (2)\]

\[\text{Also, y} = x \tan \alpha - \left( \frac{g x^2 \sec^2 \alpha}{2u '^2} \right) . . . (3)\]

\[\text{Here, y} = 0 \]

\[ \therefore \tan \alpha = e \tan \theta\]

\[ \Rightarrow \sec^2 \alpha = 1 + e^2 \tan^2 \theta\]

\[\text{and }u '^2 = u^2 \cos^2 \theta + e^2 u^2 \sin^2 \theta\]
Putting the above calculated values in equation (3), we get:
 \[\text{xe } tan\theta = \frac{g x^2 (1 + e^2 \tan^2 \theta)}{2 u^2 ( \cos^2 \theta + e^2 \sin^2 \theta)}\]

\[\text{ or, x } = \frac{2e u^2 \tan \theta ( \cos^2 \theta + e^2 \sin^2 \theta)}{g(1 + e^2 \tan^2 \theta)}\]

\[ \Rightarrow x = \frac{2e u^2 \tan \theta . \cos^2 \theta}{g}\]

\[ \Rightarrow x = \frac{e u^2 \sin 2\theta}{g}\]
Thus, from the starting point the projectile makes its second collision with the field at a distance,

\[x' = \frac{u^2 \sin 2\theta}{g} + \frac{e u^2 \sin 2\theta}{g}\]

\[ \Rightarrow x' = \frac{u^2 \sin 2\theta}{g}(1 + e)\]

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Chapter 9: Centre of Mass, Linear Momentum, Collision - Exercise [Page 162]

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HC Verma Concepts of Physics Vol. 1 [English] Class 11 and 12
Chapter 9 Centre of Mass, Linear Momentum, Collision
Exercise | Q 43 | Page 162
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