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in Physics by (68.8k points)

 A small block of mass m and concave mirror of radius R fitted with a stand, lie on a smooth, horizontal table with a separation d between them. The mirror together with its stand has a mass m. The block is pushed at t=0 towards the mirror so that it starts moving towards the mirror at speed V and collides with it. The collision is perfectly elastic.  

Find the velocity of the image 

1) at a time t< d/V 

(a)R2 V/[2(d-Vt)-R]

(b) R2 V/[2(d+ Vt)-R]

(c)R2V/[2(d-Vt)-R]2 

(d) RV [1+ R2/[2(Vt-d)-R]

 2) at a time t>d/v 

(a)R2 V/[2(d-Vt)-R]

(b) R2 V/[2(d+ Vt)-R]

(c)R2V/[2(d-Vt)-R]

(d) RV[1+ R2/[2(Vt-d)-R] 

1 Answer

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Best answer

 (1) t < (d/V) 

u = - (d- Vt) 

f = -R/2 

We know that VI/m = -m2 VO/m 

Here,m = f/ (f-u) 

m = (-R/2)/[(-R/2)+(d-Vt)] 

m = (-R)/[2(d-Vt)-R] 

Velocity of image= VI/m = -m2 VO/m 

VI= R2 V/[2(d-vt)-R]2 

(2) t > (d/v) 

Block will collide with mirror assembly after time T = d/V. From conservation of linear momentum, block and mirror assembly will exchange their momentum i.e., block will stop and mirror starts moving with velocity V. 

 U = -V [t-(d/V)] 

Also,                       m = f/(f- u) = [-R/2]/[(-R/2)+V(t-(d/V))] 

We know that VI/m = -m2VO/m VI –Vm = -m2VO/m 

Let us assume rightward direction as positive VI –Vm =-m2(-V)        or       VI = (1+m2)V 

VI=V[1+{R2/2(Vt-d)-R2}] 

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