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.
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 α−a2cosα
= g sin α - mg sinα cos2αM + m = g sinα[1−m 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