Step 1: Write the sliding condition for a block on an inclined plane.
A block slides when \( mg\sin\theta \geq \mu_s\,mg\cos\theta \), i.e., \( \tan\theta \geq \mu_s \). The mass m cancels from both sides completely.
Step 2: Apply to all three masses.
Since \( \mu_s \) is the same for all and mass does not appear in the sliding condition, all three masses begin sliding at the same critical angle \( \theta_c = \arctan(\mu_s) \). \[ \boxed{M_1,\,M_2\text{ and }M_3\text{ begin to slide at the same inclination angle}} \]