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Question: A monkey of mass \(m\) climbs a rope slung over a light frictionless pulley. The opposite end of the...

A monkey of mass mm climbs a rope slung over a light frictionless pulley. The opposite end of the rope is tied to a block of mass MM lying on a smooth horizontal plane. Then the acceleration of block when monkey moves upwards with an acceleration a'a' relative to rope is

Explanation

Solution

When the monkey is climbing up on the rope. The rope will be sliding down because of the weight of the monkey. Therefore, there will be an acceleration of the monkey and the acceleration of the rope. The relative acceleration is the vector difference of these two accelerations. Use the concept of relative acceleration to calculate the acceleration of monkeys.

Complete step by step answer: Observe the diagram:

Let point A be the position of monkey.
Let the mass of the monkey be mm
Let the acceleration of monkey be am{a_m}
Let point B is the position of the block
The mass of the block is MM
When the monkey would climb up, the force exerted by the monkey to go up will cause the block to move. Let the acceleration of the block be a0{a_0}
Acceleration of the block will be the acceleration of the rope as the block will move with the rope.
Let the acceleration in the rope be ar{a_r}
ar=a0\Rightarrow {a_r} = {a_0}
Let the acceleration of the monkey relative to the rope be amr{a_{mr}}
According to the concept of relative motion,
amr=amar{a_{mr}} = {a_m} - {a_r} . . . (1)
It is given to us that the relative acceleration of the monkey with respect to the rope is aa
amr=a\Rightarrow {a_{mr}} = a
Therefore, from equation (1), we get
a=am(a0)a = {a_m} - ( - {a_0}) (ar=a0)\left( {\because {a_r} = {a_0}} \right) . . . (2)
a=am+a0a = {a_m} + {a_0}
Rearranging it we can write
am=aa0{a_m} = a - {a_0}
Force applied is given by
F=maF = ma
Where,
FF is force applied
mm is mass of the body
aa is acceleration of the body
Now, we know that the force exerted on the block B is equal to the tension applied on the rope.
F=Ma0=T\Rightarrow F = M{a_0} = T . . . (3)
Where,
TT is tension on the rope.
Using the same concept, we can say that the force applied on the monkey due to the acceleration am{a_m} is equal to the difference of tension on the rope and the weight of the monkey.
Let Fm{F_m} be the force with which the monkey is accelerating upwards.
Fm=Tmg=mam\Rightarrow {F_m} = T - mg = m{a_m}
Tmg=m(aa0)\Rightarrow T - mg = m(a - {a_0}) (am=aa0)\left( {\because {a_m} = a - {a_0}} \right)
Rearranging it we can write
T=m(aa0)+mgT = m(a - {a_0}) + mg . . . (4)
Comparing the values of TT from equation (3) and equation (4), we can write
Ma0=m(aa0)+mgM{a_0} = m(a - {a_0}) + mg
Rearranging it we can write
Ma0=mama0+mgM{a_0} = ma - m{a_0} + mg
Ma0+ma0=ma+mg\Rightarrow M{a_0} + m{a_0} = ma + mg
(M+m)a0=m(a+g)\Rightarrow (M + m){a_0} = m(a + g)
a0=m(a+g)(M+m)\Rightarrow {a_0} = \dfrac{{m(a + g)}}{{(M + m)}}
Therefore, from the above explanation, we can conclude that the acceleration of the block is a0=m(a+g)(M+m){a_0} = \dfrac{{m(a + g)}}{{(M + m)}}

Note: Acceleration, force, tension etc are vector quantities, using them need the use of their magnitude as well as direction. We cannot use one and not the other. In this question, we have considered all the quantities moving up to be positive and all the quantities moving from left to right to be positive. Therefore, the acceleration of rope at point A, in equation (2), is negative as the rope is accelerating downwards.