Step 1: By the symmetry of projectile motion, when the object lands back at the same height it was launched from, its vertical velocity has the same magnitude as at launch but points downward, so \( v_y(\text{landing}) = -u\sin\alpha \).
Step 2: Apply the first equation of motion for the vertical direction, \( v_y = u\sin\alpha - gt \), and substitute the landing condition: \( -u\sin\alpha = u\sin\alpha - gt \).
Step 3: Solve for \( t \): \( gt = u\sin\alpha + u\sin\alpha = 2u\sin\alpha \).
\[ \boxed{t = \dfrac{2u\sin\alpha}{g}} \]