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A projectile is fired with a velocity \( u \) at right angle to
P the plane, which is inclined at angle \( \theta \) with the

W horizontal. The horizontal displacement along \( x \) of the projectile is
(1) \( \frac{u^{2}}{g} \tan \theta \)
(2) \( \frac{2 u^{2}}{g} \tan \theta \)
(3) \( \frac{u^{2}}{2 g} \tan \theta \)
(4) \( \frac{u^{2}}{g^{2}} \tan \theta \)
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