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The masses and radii of the Earth and th...

The masses and radii of the Earth and the Moon are `M_1, R_1 and M_2,R_2` respectively. Their centres are at a distance d apart. The minimum speed with which a particle of mass m should be projected from a point midway between the two centres so as to escape to infinity is ........

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To solve the problem of finding the minimum speed with which a particle of mass \( m \) should be projected from a point midway between the Earth and the Moon so as to escape to infinity, we can use the principle of conservation of mechanical energy. ### Step-by-Step Solution: 1. **Identify the Initial Conditions**: - The particle is projected from the midpoint between the Earth and the Moon. The distance between the centers of the Earth and Moon is \( d \). - Therefore, the distance from the midpoint to the center of the Earth is \( \frac{d}{2} \) and the same applies to the distance to the center of the Moon. 2. **Calculate the Initial Potential Energy**: - The gravitational potential energy \( U \) between two masses \( M \) and \( m \) separated by a distance \( r \) is given by: \[ U = -\frac{G M m}{r} \] - For the particle at the midpoint, the potential energy due to the Earth is: \[ U_1 = -\frac{G M_1 m}{\frac{d}{2}} = -\frac{2 G M_1 m}{d} \] - The potential energy due to the Moon is: \[ U_2 = -\frac{G M_2 m}{\frac{d}{2}} = -\frac{2 G M_2 m}{d} \] - Therefore, the total initial potential energy \( U_i \) is: \[ U_i = U_1 + U_2 = -\frac{2 G M_1 m}{d} - \frac{2 G M_2 m}{d} = -\frac{2 G (M_1 + M_2) m}{d} \] 3. **Final Conditions at Infinity**: - At infinity, the potential energy \( U_f \) is zero, and we assume the kinetic energy \( K_f \) is also zero for the minimum speed case (the particle just escapes). - Thus, the total mechanical energy at infinity is: \[ E_f = K_f + U_f = 0 + 0 = 0 \] 4. **Apply Conservation of Mechanical Energy**: - According to the conservation of mechanical energy: \[ E_i = E_f \] - Therefore: \[ K_i + U_i = 0 \] - The initial kinetic energy \( K_i \) is given by: \[ K_i = \frac{1}{2} m v_0^2 \] - Substituting the initial potential energy: \[ \frac{1}{2} m v_0^2 - \frac{2 G (M_1 + M_2) m}{d} = 0 \] 5. **Solve for Minimum Speed \( v_0 \)**: - Rearranging the equation gives: \[ \frac{1}{2} m v_0^2 = \frac{2 G (M_1 + M_2) m}{d} \] - Dividing both sides by \( m \) (assuming \( m \neq 0 \)): \[ \frac{1}{2} v_0^2 = \frac{2 G (M_1 + M_2)}{d} \] - Multiplying both sides by 2: \[ v_0^2 = \frac{4 G (M_1 + M_2)}{d} \] - Taking the square root: \[ v_0 = \sqrt{\frac{4 G (M_1 + M_2)}{d}} = \frac{2 \sqrt{G (M_1 + M_2)}}{\sqrt{d}} \] ### Final Answer: The minimum speed with which a particle of mass \( m \) should be projected from the midpoint between the Earth and the Moon to escape to infinity is: \[ v_0 = \frac{2 \sqrt{G (M_1 + M_2)}}{\sqrt{d}} \]

To solve the problem of finding the minimum speed with which a particle of mass \( m \) should be projected from a point midway between the Earth and the Moon so as to escape to infinity, we can use the principle of conservation of mechanical energy. ### Step-by-Step Solution: 1. **Identify the Initial Conditions**: - The particle is projected from the midpoint between the Earth and the Moon. The distance between the centers of the Earth and Moon is \( d \). - Therefore, the distance from the midpoint to the center of the Earth is \( \frac{d}{2} \) and the same applies to the distance to the center of the Moon. ...
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