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Two bodies, each of mass M, are kept fix...

Two bodies, each of mass M, are kept fixed with a separation 2L. A particle of mass m is projected from the midpoint of the line joining their cehntres, perpendicualr to the line. The gravitational constant is G. The correct statement (s) is (are)

A

(a)The minimum initial velocity of the mass m to escape the gravitational field of the two bodies is `4sqrt((GM)/L)`

B

The minimum initial velocity of the mass m to escape the gravitational field of the two bodies is `2sqrt((GM)/L)`

C

The minimum initial velocity of the mass m to escape the gravitational field of the two bodies is `sqrt((2GM)/L)`

D

The energy of the mass m remains constant.

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To solve the problem, we need to determine the minimum initial velocity required for a particle of mass \( m \) to escape the gravitational influence of two fixed bodies, each of mass \( M \), separated by a distance of \( 2L \). The particle is projected from the midpoint of the line joining the centers of the two masses. ### Step-by-Step Solution: 1. **Identify the Setup**: - We have two masses \( M \) located at points \( A \) and \( B \) with a separation of \( 2L \). - The midpoint, where the mass \( m \) is projected, is at a distance \( L \) from each mass. 2. **Calculate the Gravitational Potential Energy**: - The gravitational potential energy \( U \) between two masses is given by: \[ U = -\frac{G M m}{r} \] - At the midpoint, the distance from mass \( M \) at \( A \) to mass \( m \) is \( L \) and similarly for mass \( B \). - Therefore, the total potential energy \( U \) at the midpoint is: \[ U = -\frac{G M m}{L} - \frac{G M m}{L} = -\frac{2GMm}{L} \] 3. **Set Up the Energy Conservation Equation**: - The total mechanical energy \( E \) at the starting point (where the particle is projected) must equal the total mechanical energy at infinity (where it escapes the gravitational influence). - At infinity, the potential energy is \( 0 \) and the kinetic energy is also \( 0 \) (as the particle just escapes). Thus, the total energy at infinity is: \[ E_{\text{final}} = 0 \] - At the midpoint, the total energy is the sum of kinetic energy \( K \) and potential energy \( U \): \[ E_{\text{initial}} = K + U = \frac{1}{2} mv^2 - \frac{2GMm}{L} \] - Setting the initial energy equal to the final energy: \[ \frac{1}{2} mv^2 - \frac{2GMm}{L} = 0 \] 4. **Solve for the Initial Velocity \( v \)**: - Rearranging the equation gives: \[ \frac{1}{2} mv^2 = \frac{2GMm}{L} \] - Dividing both sides by \( m \) (assuming \( m \neq 0 \)): \[ \frac{1}{2} v^2 = \frac{2GM}{L} \] - Multiplying both sides by \( 2 \): \[ v^2 = \frac{4GM}{L} \] - Taking the square root: \[ v = 2\sqrt{\frac{GM}{L}} \] 5. **Conclusion**: - The minimum initial velocity required for the mass \( m \) to escape the gravitational field of the two bodies is: \[ v = 2\sqrt{\frac{GM}{L}} \]

To solve the problem, we need to determine the minimum initial velocity required for a particle of mass \( m \) to escape the gravitational influence of two fixed bodies, each of mass \( M \), separated by a distance of \( 2L \). The particle is projected from the midpoint of the line joining the centers of the two masses. ### Step-by-Step Solution: 1. **Identify the Setup**: - We have two masses \( M \) located at points \( A \) and \( B \) with a separation of \( 2L \). - The midpoint, where the mass \( m \) is projected, is at a distance \( L \) from each mass. ...
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