Step 1: Write the horizontal and vertical positions as functions of time: \( x = (u\cos\alpha)t \) and \( y = (u\sin\alpha)t - \dfrac{1}{2}gt^2 \).
Step 2: From the horizontal equation, solve for time in terms of position, \( t = \dfrac{x}{u\cos\alpha} \), then substitute this into the vertical equation to eliminate \( t \) and express \( y \) purely in terms of \( x \).
Step 3: The projectile lands when \( y = 0 \) again (other than at the launch point \( x = 0 \)). Setting the resulting expression to zero and solving for the nonzero value of \( x \) gives \( R = \dfrac{2u^2\sin\alpha\cos\alpha}{g} \), which simplifies using the double-angle identity \( 2\sin\alpha\cos\alpha = \sin 2\alpha \).
\[ \boxed{R = \dfrac{u^2\sin 2\alpha}{g}} \]