Step 1: At launch, the projectile has total kinetic energy \( \dfrac{1}{2}mu^2 \). At the highest point, the vertical velocity is zero and only the horizontal component \( u\cos\alpha \) remains, so the kinetic energy there is \( \dfrac{1}{2}m(u\cos\alpha)^2 \), plus the gained potential energy \( mgH \).
Step 2: Apply conservation of energy between launch and the highest point: \( \dfrac{1}{2}mu^2 = \dfrac{1}{2}m(u\cos\alpha)^2 + mgH \).
Step 3: Cancel the mass \( m \) and solve for \( H \): \( gH = \dfrac{1}{2}u^2(1 - \cos^2\alpha) = \dfrac{1}{2}u^2\sin^2\alpha \), using the identity \( 1 - \cos^2\alpha = \sin^2\alpha \).
\[ \boxed{H = \dfrac{u^2\sin^2\alpha}{2g}} \]