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Question: A cart of mass \[M\] has a block of mass \[m\] in contact with it as shown in the figure. The coeffi...

A cart of mass MM has a block of mass mm in contact with it as shown in the figure. The coefficient of friction between the block and the cart is μ\mu . What should be the minimum acceleration of the cart so that the block of mass mm does not fall?

Explanation

Solution

In this question, let us assume the cart of mass MM moves with an acceleration a m/s2a{\text{ m/}}{{\text{s}}^2}. Thus, a pseudo force mama acts on the small block of mass mm and it must be equal to the normal force between the blocks for horizontal equilibrium. The force of friction μN\mu N will act in the upward direction and must be equal to mgmg so that the block does not fall. From this condition, we can find out the minimum acceleration required.

Formula used:
F=maF = ma
Where FF is the total force, mm is the mass of the system and aa is the net acceleration of the system.
f=μNf = \mu N
Where, ff is the limiting frictional force, μ\mu is the coefficient of friction and NN is the normal force acting.

Complete step by step answer:
Let us assume the cart of mass MM is moving with an acceleration of a m/s2a{\text{ m/}}{{\text{s}}^2}. It is in contact with a block of mass mm such that the coefficient of friction between the cart and block is μ\mu . A normal force NN acts on the block in the horizontal direction.As the cart is accelerating a pseudo force F=maF = ma acts in the opposite direction of acceleration
For horizontal equilibrium,
N=F=maN = F = ma

Frictional force f=μNf = \mu N acts in the upward direction. For block to be in equilibrium frictional force must balance its weight,
fmgf \geqslant mg
μNmg\Rightarrow \mu N \geqslant mg
Substituting N=F=maN = F = ma,
μmamg\Rightarrow \mu ma \geqslant mg
agμ\therefore a \geqslant \dfrac{g}{\mu }

Thus, minimum acceleration so that the block does not fall must be gμ m/s2\dfrac{g}{\mu }{\text{ m/}}{{\text{s}}^2}.

Note: Pseudo force is an imaginary force like frictional force and comes in effect when the frame of reference has started acceleration compared to a non-accelerating frame. It always acts in the opposite direction of the motion. The work done by a pseudo force is zero as it acts to appear on the body.