Properties Of Matter Ques 18

  1. A ball of density $d$ is dropped on to a horizontal solid surface. It bounces elastically from the surface and returns to its original position in a time $t_1$. Next, the ball is released and it falls through the same height before striking the surface of a liquid of density $d_L$.

(1992, 8 M)

(a) If $d<d_L$, obtain an expression (in terms of $d, t_1$ and $d_L$ ) for the time $t_2$ the ball takes to come back to the position from which it was released.

(b) Is the motion of the ball simple harmonic ?

(c) If $d=d_L$, how does the speed of the ball depend on its depth inside the liquid? Neglect all frictional and other dissipative forces. Assume the depth of the liquid to be large

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Answer:

Correct Answer: 18.(a) $\frac{t_1 d_L}{d_L-d}$ (b) no (c) remains same.

Solution:

  1. In elastic collision with the surface, direction of velocity is reversed but its magnitude remains the same. Therefore, time of fall $=$ time of rise or time of fall $=\frac{t_1}{2}$

Hence, velocity of the ball just before it collides with liquid is

$ v=g \frac{t_1}{2} $

Retardation inside the liquid,

$ a=\frac{\text { upthrust }- \text { weight }}{\text { mass }}=\frac{V d_L g-V d g}{V d}=\left(\frac{d_L-d}{d}\right) g \ldots $

Time taken to come to rest under this retardation will be

$ t=\frac{\nu}{a}=\frac{g t_1}{2 a}=\frac{g t_1}{2\left(\frac{d_L-d}{d}\right) g}=\frac{d t_1}{2\left(d_L-d\right)} $

Same will be the time to come back on the liquid surface. Therefore,

(a) $t_2=$ time the ball takes to came back to the position from where it was released $ =t_1+2 t=t_1+\frac{d t_1}{d_L-d}=t_1\left[1+\frac{d}{d_L-d}\right] \text { or } t_2=\frac{t_1 d_L}{d_L-d} $

(b) The motion of the ball is periodic but not simple harmonic because the acceleration of the ball is $g$ in air and $\left(\frac{d_L-d}{d}\right) g$ inside the liquid which is not proportional to the displacement, which is necessary and sufficient condition for SHM.

(c) When $d_L=d$, retardation or acceleration inside the liquid becomes zero (upthrust $=$ weight). Therefore, the ball will continue to move with constant velocity $v=g t_1 / 2$ inside the liquid.



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