Two projectiles are launched with identical initial speeds at angles \( (45^\circ + \alpha) \) and \( (45^\circ - \alpha) \) relative to the horizontal. The formula for the time of flight \( T \) of a projectile is \( T = \frac{2u \sin \theta}{g} \), where \( u \) is the initial speed, \( \theta \) is the launch angle, and \( g \) is the acceleration due to gravity.
Step 1: Time of flight for the first projectile
The first projectile is launched at an angle \( (45^\circ + \alpha) \). Its time of flight \( T_1 \) is calculated as:
\[ T_1 = \frac{2u \sin(45^\circ + \alpha)}{g} \]
Applying the sine angle addition identity:
\[ T_1 = \frac{2u (\sin 45^\circ \cos \alpha + \cos 45^\circ \sin \alpha)}{g} \]
Substituting \( \sin 45^\circ = \cos 45^\circ = \frac{1}{\sqrt{2}} \):
\[ T_1 = \frac{2u \left(\frac{1}{\sqrt{2}} (\cos \alpha + \sin \alpha) \right)}{g} \]
Step 2: Time of flight for the second projectile
The second projectile is launched at an angle \( (45^\circ - \alpha) \). Its time of flight \( T_2 \) is:
\[ T_2 = \frac{2u \sin(45^\circ - \alpha)}{g} \]
Applying the sine angle subtraction identity:
\[ T_2 = \frac{2u (\sin 45^\circ \cos \alpha - \cos 45^\circ \sin \alpha)}{g} \]
Substituting \( \sin 45^\circ = \cos 45^\circ = \frac{1}{\sqrt{2}} \):
\[ T_2 = \frac{2u \left(\frac{1}{\sqrt{2}} (\cos \alpha - \sin \alpha) \right)}{g} \]
Step 3: Ratio of the times of flight
The ratio of the times of flight \( T_1 \) to \( T_2 \) 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 yields:
\[ \frac{T_1}{T_2} = \frac{\cos \alpha + \sin \alpha}{\cos \alpha - \sin \alpha} \]
Dividing the numerator and denominator by \( \cos \alpha \) and using the identity \( \tan \alpha = \frac{\sin \alpha}{\cos \alpha} \), the ratio becomes:
\[ \frac{T_1}{T_2} = \frac{1 + \tan \alpha}{1 - \tan \alpha} \]
The correct answer is option (4): \( \frac{1 + \tan \alpha}{1 - \tan \alpha} \).