Imagine a situation in which the given arrangement is placed inside an elevator that can move only in the vertical direction and compare the situation with the case when it is placed on the ground if the elevator accelerates downward with ao(< g)
the system does not accelerate with respect to the elevator unless m >
Draw the Free body diagram in the lifts frame
(Mao is the pseudo force)
∴∑Fy=0
∴ N = (Mg - Mao) (given ao< g)
= M(g - ao)
We can see that the normal force reduces from Mg to M(g - ao)
∴ limiting friction will reduce
∴N=(Mg−Mao) (given ao<g)
∴ = M(g-ao)
We can see that the normal force reduces from Mg to M(g-ao)
∴ Limiting friction will reduce
Let us assume, the system is accelerated.
Then, T-f =Ma (∑Fx)
Mg - mao -T = ma (∑Fy)
m(g - ao) - f = (m+M)a
If they are accelerating,then f=fmax = μN=μ M(g-ao)
∴ m(g-ao) - μ M(g-ao)= (m+M)a
⇒a = g−aom+M(m - μM)
∴For acceleration to occur,
m>μM as a constant be negative.