Taking reference line through support, S let xA and xB are the distances of blocks A and B, respectively, from S. The total length of the string.
l=4xA+5xB+l0, where l0 is some part of string which is over pulley and somewhere else which remains constant. Differentiating l w.r.t. time, we get
dldt=ddt(4xA+5xB+l0)
or o=4dxAdt+5dxBdt⇒dxAdt=54dxBdt
dxAdt=−vA (-because xa is decreasing with time)
dxBdt=−vB (+because xb is increasing with time)
or vA=54vB; also aA=54aB
Method 2:
Charge in the length of segment I, Δl1,2=0+(xB)
Segment II
Δl3,4=(−xA)+(xB)
Segment III
Δl5,6=(−xA)+(xB)
Segment IV
Δl7,8=(−xA)+(xB)
Segment V
Δl9,10=(−xA)+(xB)
Total charge in segment lengths should be zero.Therefore,
Δl=Δl1,2+Δl3,4+Δl5,6+Δl7,8+Δl9,10=0
=xB+[−xA+xB]+[−xA+xB]+[−xA+xB]+[−xA+xB]=0
=−4xA+5xB=0
or xA=54xB⇒vA=54vB⇒aA=54aB
Equations of motion
For A :
4T=mAaA=MaA..........(i)
For B :
F−5T=mBaB=3MaB.......(ii)
aB=16F73
and
aA=54×(16F73)=20F73
![1030008_985010_ans_4da14dbed1794dc285cde1586a31c06e.PNG](https://search-static.byjusweb.com/question-images/toppr_invalid/questions/1030008_985010_ans_4da14dbed1794dc285cde1586a31c06e.PNG)