Step 1: Let the body of mass \( m \) slide a distance \( s \) down the smooth incline, starting from rest. The vertical height it drops through is \( h = s\sin\theta \).
Step 2: Since the incline is frictionless, mechanical energy is conserved: the loss in potential energy converts entirely into kinetic energy. \[ mgh = \frac{1}{2}mv^2 \implies v^2 = 2g\sin\theta \cdot s \]
Step 3: Compare this with the standard kinematic relation \( v^2 = 2as \) for motion starting from rest. Matching the two expressions for \( v^2 \) gives \( 2as = 2g\sin\theta \cdot s \), so the acceleration works out to: \[ \boxed{a = g\sin\theta} \]