We are given two projectiles that are fired at angles \( (45^\circ + \alpha) \) and \( (45^\circ - \alpha) \) with the horizontal direction. Both projectiles have the same initial speed.
The time of flight \( T \) for a projectile is given by the formula: \[ T = \frac{2u \sin \theta}{g} \] where: \( u \) is the initial speed, \( \theta \) is the angle of projection, \( g \) is the acceleration due to gravity.
Step 1: Time of flight for the first projectile
For the first projectile, the angle of projection is \( (45^\circ + \alpha) \), so the time of flight \( T_1 \) is: \[ T_1 = \frac{2u \sin(45^\circ + \alpha)}{g} \] Using the angle addition identity for sine: \[ T_1 = \frac{2u (\sin 45^\circ \cos \alpha + \cos 45^\circ \sin \alpha)}{g} \] \[ T_1 = \frac{2u \left(\frac{1}{\sqrt{2}} (\cos \alpha + \sin \alpha) \right)}{g} \]
Step 2: Time of flight for the second projectile
For the second projectile, the angle of projection is \( (45^\circ - \alpha) \), so the time of flight \( T_2 \) is: \[ T_2 = \frac{2u \sin(45^\circ - \alpha)}{g} \] Using the angle subtraction identity for sine: \[ T_2 = \frac{2u (\sin 45^\circ \cos \alpha - \cos 45^\circ \sin \alpha)}{g} \] \[ T_2 = \frac{2u \left(\frac{1}{\sqrt{2}} (\cos \alpha - \sin \alpha) \right)}{g} \]
Step 3: Ratio of the times of flight
The ratio of the times of flight \( T_1 \) and \( T_2 \) is: \[ \frac{T_1}{T_2} = \frac{\frac{2u \left(\frac{1}{\sqrt{2}} (\cos \alpha + \sin \alpha) \right)}{g}}{\frac{2u \left(\frac{1}{\sqrt{2}} (\cos \alpha - \sin \alpha) \right)}{g}} \] Simplifying the expression: \[ \frac{T_1}{T_2} = \frac{\cos \alpha + \sin \alpha}{\cos \alpha - \sin \alpha} \] Using the identity \( \frac{1 + \tan \alpha}{1 - \tan \alpha} \), we find that the ratio of the times of flight is: \[ \frac{1 + \tan \alpha}{1 - \tan \alpha} \]
Thus, the correct answer is option (4): \( \frac{1 + \tan \alpha}{1 - \tan \alpha} \).