In the arrangement shown in the fig., the ends P and Q of an un-stretchable string move downwards with uniform speed U. Pulleys A and B are fixed. Mass M moves upwards with a speed?
U/cosθ
The block will obviously go up and that too vertically up as both sides are pulled with same velocity.
Lets assume block is going up by velocity v
Now focus on one string.
Now AB is the string between pulley and block M
AB is being pulled by velocity U and if M block is fixed then the string will stretch which cannot happen as ideal strings are non elastic.
Now here since the block is going up with velocity v then its component V cos θ will be towards the string.
Now for the block to go up such that the string is to neither stretch or break or slacken so U = vcosθ ⇒ U = Ucosθ
Alternate solution:
From the triangle MNO, using Pythagoras theorem
MN2 + NO2 = MO2
∴ x2 + z2 = L2
Here x is a constant.
Differentiating the above equation by t:
0 + 2zdzdt = 2ldldt(as MN distance is always constant so dxdt = 0)
⇒ VM = Iz.U
VM = lzU = Uzl = Ucosθ(∵ cosθ = zl)