In the given situation, two blocks A and B are arranged as shown in the figure. M is a fixed pulley and N is a movable pulley. The system is released from rest. What is the relationship between accelerations for the blocks A and B?
aB = -2aA
Let us consider the system shown in the figure. It is clear from the figure that the position of A is governed by the position of centre of movable pulley. Let at any instant the block B is at yB and center of movable pulley is yA from the reference line (dotted line). The total length of the cord:
YB+2YA=I0 ............(i)
I0 is the length of the string (remain constant). Assume acceleration of blocks and pulleys. Differentiating equation (i) with respect to time, we get
dyBdt+2dyAdt=dl0dt ............(ii)
As i0 is constant, dl0dt=0
and dyBdt=vB and dyAdt=−vA
as YA is decreasing since block A is assumed tobe with acceleration aA
the equation (ii) become vB−2vA=0 ...........(iii)
Differentiating once more we get aB−2aA=0 or aB=+2aA
This means block B goes down with twice the acceleration with which A goes upwards. ⇒aB=−2aA
Alternate solution II If mass A goes up by a distance x, we can observe that the string lengths ab and cd are slack. Due to the weight of block B, this length (ab + cd = 2x) will go on this side and block B, will descend by a distance 2x. As in equal time duration,
B has travelled a distance twice that of A. So vB=−2vA and aB=−2aA
Alternate solution III
Displacement of the pulley is the average displacement of both sides of the pulley.
⇒xA=xp+02
⇒xP=2xA
Now for pulley 2
0=xP−xB2
XP=XB
⇒2XA=XB Lets take care of direction
A goes up so xA is +ve
B goes down so XB is -ve
XB=−2XA
VB=−2VA
aB=−2aA