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Question

A block of mass m is placed on a triangular block of mass M, which in turn is placed on a horizontal smooth surface as shown in figure. Assuming frictionless surfaces, find the velocity of the triangular block when the smaller block reaches the bottom end.


A

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B

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C

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D

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Solution

The correct option is B


The block 'm' will slide down the inclined plane of mass M with acceleration a1 g sin α (relative) to the inclined plane.

The horizontal component of a1 will be, ax=g sin αcosα, for which the block M will accelerate towards left, Let, the acceleration be a2.

According to the concept of centre of mass, (in the horizontal direction external force is zero).

max=(M+m)a2

a2 = maxM+m = mg sin αcosαM+m .......(1)

So, the absolute ( Resultant) acceleration of 'm' on the block 'M' along the direction of the inclinie will be.

a = g sin αa2cosα

= g sin α - mg sinα cos2αM + m = g sinα[1m cos2αM + m]

= g sin α [M + m cos2αM + m]

So, a = g sin α [M + msin4αM +m] ........ (2)

Let, the time taken by the block 'm' to reach the bottom end be 't'.

Now, S=ut+(12)at2

hsinα=(12) at2 = 2a sinα

So, the velocity of the bigger block after time ' t' will be.

Vm = u + a2t = mg sinα cosαM + m 2a sinα = 2m2 g2 h sin2α cos2α(M + m)2 a sinα

Now, subtracting the value of a from equation (2), we get,

Vm = [2m2 g2 h sin2α cos2α(M + m)2 sinα×(M + m)g sinα (M = m sin2α]12

or Vm = [2m2 g2 h cos2α(M + m) (M + m sin2α)]12


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