In this case, the block on the floor is being pulled horizontally by the block hanging vertically. The force of static friction is what prevents the block from moving. The frictional force must balance the horizontal force exerted by the tension in the string, which is equal to the weight of the hanging block.
From the equilibrium condition:
\[
T = M g \sin \theta
\]
The frictional force \( f \) is given by:
\[
f = \mu M g \cos \theta
\]
At equilibrium, \( f = T \), so:
\[
\mu M g \cos \theta = M g \sin \theta
\]
Canceling out \( M g \) from both sides:
\[
\mu \cos \theta = \sin \theta
\]
Thus, the coefficient of static friction is:
\[
\mu = \tan \theta
\]