This question asks for the correct formula for the horizontal range of a projectile launched at angle \( \alpha \) with speed \( u \). Rather than re-deriving it from scratch, let's test each option against known physical behavior of projectile range.
- \( R = \dfrac{u^2\cos 2\alpha}{g} \): Using \( \cos 2\alpha \), the range would be maximum at \( \alpha = 0^\circ \) (a purely horizontal launch) and would actually turn negative for angles above 45°, which contradicts the well-known fact that a projectile achieves its maximum range at a 45° launch angle, not at 0°.
- \( R = \dfrac{u^2\sin 2\alpha}{g} \): The function \( \sin 2\alpha \) reaches its peak value of 1 exactly when \( 2\alpha = 90^\circ \), that is, when \( \alpha = 45^\circ \). This matches the well-established physical result that a projectile travels the farthest horizontal distance when launched at 45° to the horizontal, for a fixed launch speed.
- \( R = \dfrac{u^2\cos\alpha}{g} \): This expression would be maximum at \( \alpha = 0^\circ \), predicting that launching perfectly horizontally gives the farthest range, which does not correctly represent range as a function of launch angle in projectile motion.
- \( R = \dfrac{u^2\sin\alpha}{g} \): This form would keep increasing all the way up to \( \alpha = 90^\circ \) (a straight vertical launch), which is physically wrong since a projectile launched straight up travels zero horizontal distance, not the maximum.
Only the option using \( \sin 2\alpha \) correctly predicts that the range peaks at a 45° launch angle and returns to zero at both 0° and 90°, matching the true behavior of projectile range.
Therefore, the correct answer is \( R = \dfrac{u^2\sin 2\alpha}{g} \).