In case (a), let Y be Young's modulus of the material of the
wire. If a is its area of cross section, then we can write
Y=F/al/LF/al/L=Wlal(∵F=W)
Increaseinlengthofwirel=WLaY
In case (b), we can treat either segment of length L/2
in Fig. 5] 7(b) as if one of its ends is fixed while the other end is
attached to the load W because the point M remains stationary, i.e.,
fixed all the time due to symmetrical load. Thus, when the wire is
passed over the pulley, let l be the increase in the length of each
segment. Since each segment is of length L/2, we have
Y=W(L/2)al′
Increase in length of wire of one side of pulley
Therefore, increase in length of both the segments of the wire
=l′+l′=l/2+l/2=l
So the increase in length remains the same.