The coefficient of static friction between the two blocks shown in figure is μ and the table is smooth. What maximum horizontal force F can be applied to the block of mass M so that the blocks move together?
When the maximum force F is applied, both the blocks move together towards right. The only horizontal force on the upper block of mass m is that due to the friction by the lower block of mass M. Hence this force on m should be towards right. The force of friction on M by m should be towards left by Newton's third law. As we are talking of the maximum possible force F that can be applied, the friction is limiting and hence f = μN , where N is the normal force between the blocks.
Consider the motion of m. The forces on m are,
(a) mg downward by the earth (gravity),
(b) N upward by the block M (normal force) and
(c) f = μN (friction) towards right by the block M.
In the vertical direction, there is no acceleration. This gives
N = mg . . . . . .(i)
In the horizontal direction, let the acceleration be a, then
μN = m a
or, μmg = ma
or, a = μg . . . . . .(ii)
Next, consider the motion of M
The forces on M are
(a) Mg downward by the earth (gravity),
(b) N1 upward by the table (normal force),
(c) N downward by m (normal force),
(d) f=μN (friction) towards left by m and
(e) F (applied force) by the experimenter.
The equation of motion is
F - μN = M a
or, F - μmg = M μg [Using (i) and (ii)]
or, F = μg (M + m)