
Given that initially, the system is at rest so v
cm = 0. Now in slipping as no horizontal force is applied, the horizontal component of velocity of centre of mass of the system must remain constant. So, if v and V are the velocities of cylinder and block at B relative to the ground
(mv + MV)/(m+M) = const. = 0
i.e. mv + MV = 0 as m + M = finite ...... (1)
or m (∆r1)/∆t+(∆r2)/∆t M=0 [as v = (∆r1)/∆t]
or mΔr1 + MΔr2 = 0 as Δr1 = d
or md1 - Md2 = 0 as d2 is opposite to d1 ....... (2)
Now, when the cylinder reaches from A and B, it is displaced by a distance (R - r) horizontally to the right relative to the block. So, if the displacement of the block relative to ground is d2 to the left, the displacement of cylinder relative to ground to the right will be
d1 = (R-r) - d2 ......(3)
Substituting d1 from Equation (3) in(2), we get
M[(R-r)-d2]-md2 = 0
i.e. d2 = (m(R-r))/(M+m) (to the left)
Therefore, the distance traveled by the block when the cylinder reaches the point B is
d2 = (m(R-r))/(M+m) (to the left)