The horizontal range \( R \) of a projectile launched with initial velocity \( u \) at an angle \( \theta \) with the horizontal is given by: \[ R = \frac{u^2 \sin 2\theta}{g} \] The maximum height \( H_{max} \) attained by the projectile is given by: \[ H_{max} = \frac{u^2 \sin^2 \theta}{2g} \] We are given that the horizontal range is three times the maximum height: \[ R = 3 H_{max} \] \[ \frac{u^2 \sin 2\theta}{g} = 3 \left( \frac{u^2 \sin^2 \theta}{2g} \right) \] \[ \frac{u^2 (2 \sin \theta \cos \theta)}{g} = \frac{3 u^2 \sin^2 \theta}{2g} \] We can cancel \( \frac{u^2}{g} \) from both sides (assuming \( u \neq 0 \)): \[ 2 \sin \theta \cos \theta = \frac{3}{2} \sin^2 \theta \] Assuming \( \sin \theta \neq 0 \) (i.e., the projectile is launched at an angle other than 0 or 180 degrees), we can divide by \( \sin \theta \): \[ 2 \cos \theta = \frac{3}{2} \sin \theta \] \[ \frac{\sin \theta}{\cos \theta} = \tan \theta = \frac{2}{3/2} = \frac{4}{3} \] Now we need to find the horizontal range \( R \) in terms of \( u \) and \( g \). We know \( R = \frac{u^2 \sin 2\theta}{g} = \frac{u^2 (2 \sin \theta \cos \theta)}{g} \). If \( \tan \theta = \frac{4}{3} \),
we can consider a right-angled triangle where the opposite side is 4 and the adjacent side is 3.
The hypotenuse is \( \sqrt{4^2 + 3^2} = \sqrt{16 + 9} = \sqrt{25} = 5 \).
So, \( \sin \theta = \frac{4}{5} \) and \( \cos \theta = \frac{3}{5} \).
Substituting these values into the expression for \( R \): \[ R = \frac{u^2 (2 \times \frac{4}{5} \times \frac{3}{5})}{g} = \frac{u^2 (\frac{24}{25})}{g} = \frac{24 u^2}{25 g} \] We are given that the horizontal range is \( R = \frac{nu^2}{25g} \).
Comparing this with our result, we find that \( n = 24 \).