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A gun of mass M(including the carriage) ...

A gun of mass M(including the carriage) fires a shot of mass `m`. The gun along with the carriage is kept on a smooth horizontal surface. The muzzle speed of the bullet `v_r` is constant. Find
(a) The elevation of the gun with horizontal at which maximum range of bullet with respect to the ground is obtained.
(b) The maximum range of the bullet.

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To solve the problem, we will break it down into two parts: finding the elevation angle for maximum range and calculating the maximum range itself. ### Part (a): Finding the elevation angle for maximum range 1. **Understanding the System**: - We have a gun of mass \( M \) (including the carriage) that fires a bullet of mass \( m \). - The bullet has a muzzle speed \( v_r \) and is fired at an angle \( \theta \) with respect to the horizontal. 2. **Initial Conditions**: - Before firing, the entire system (gun + bullet) is at rest. Therefore, the initial momentum of the system is zero. 3. **Applying Conservation of Momentum**: - When the bullet is fired, the gun recoils. By conservation of momentum: \[ 0 = m v + M V_g \] where \( v \) is the velocity of the bullet and \( V_g \) is the velocity of the gun after firing. - The velocity of the bullet can be expressed as: \[ v = v_r \cos \theta + V_g \] 4. **Finding the Velocity of the Gun**: - Rearranging the momentum equation gives: \[ V_g = -\frac{m v_r \cos \theta}{M} \] 5. **Velocity of the Bullet**: - Substituting \( V_g \) back into the bullet's velocity equation: \[ v = v_r \cos \theta - \frac{m v_r \cos \theta}{M} \] - Simplifying gives: \[ v = v_r \cos \theta \left(1 - \frac{m}{M}\right) \] 6. **Time of Flight**: - The time of flight \( T \) for the bullet can be calculated using the vertical component of the bullet's velocity: \[ T = \frac{2 v_r \sin \theta}{g} \] 7. **Finding the Elevation Angle for Maximum Range**: - The horizontal range \( R \) is given by: \[ R = V_g T \] - Substituting \( V_g \) and \( T \): \[ R = -\frac{m v_r \cos \theta}{M} \cdot \frac{2 v_r \sin \theta}{g} \] - To maximize \( R \), we need to maximize \( \sin 2\theta \). This occurs at \( \theta = 45^\circ \). ### Part (b): Calculating the Maximum Range 1. **Substituting \( \theta = 45^\circ \)**: - At \( \theta = 45^\circ \), \( \sin 2\theta = 1 \). - The range becomes: \[ R = \frac{m v_r^2}{g (M + m)} \] 2. **Final Expression for Maximum Range**: - Thus, the maximum range \( R \) of the bullet is: \[ R = \frac{m v_r^2}{g (M + m)} \] ### Summary of Results: - **(a)** The elevation angle \( \theta \) for maximum range is \( 45^\circ \). - **(b)** The maximum range of the bullet is \( R = \frac{m v_r^2}{g (M + m)} \).

To solve the problem, we will break it down into two parts: finding the elevation angle for maximum range and calculating the maximum range itself. ### Part (a): Finding the elevation angle for maximum range 1. **Understanding the System**: - We have a gun of mass \( M \) (including the carriage) that fires a bullet of mass \( m \). - The bullet has a muzzle speed \( v_r \) and is fired at an angle \( \theta \) with respect to the horizontal. ...
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