Step 1: Identify the forces acting on a block on an inclined plane.
For any block of mass \(m\) placed on an inclined plane, the component of weight acting down the plane is
\[
mg\sin\theta
\]
The normal reaction on the block is
\[
N=mg\cos\theta
\]
The maximum static friction is
\[
f_{\max}=\mu_s N
\]
Therefore,
\[
f_{\max}=\mu_s mg\cos\theta
\]
Step 2: Apply the condition for just sliding.
The block begins to slide when the component of weight down the plane becomes equal to the maximum static friction.
So,
\[
mg\sin\theta=\mu_s mg\cos\theta
\]
Step 3: Simplify the equation.
Cancelling \(mg\) from both sides, we get
\[
\sin\theta=\mu_s\cos\theta
\]
Dividing by \(\cos\theta\),
\[
\tan\theta=\mu_s
\]
Hence,
\[
\theta=\tan^{-1}(\mu_s)
\]
Step 4: Understand the dependence on mass.
The angle at which sliding begins is
\[
\theta=\tan^{-1}(\mu_s)
\]
This expression does not contain mass \(m\).
Therefore, the angle of sliding is independent of the mass of the object.
Since the coefficient of static friction \(\mu_s\) is the same for \(M_1\), \(M_2\), and \(M_3\), all three masses will begin to slide at the same inclination angle.
Step 5: Final conclusion.
Therefore,
\[
\boxed{M_1,\ M_2\ \text{and}\ M_3\ \text{begin to slide at the same inclination angle}}
\]