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A satellite is revolving near by earth o...

A satellite is revolving near by earth of radius `=R_e`. If its velocity is increased `sqrt(3/2)v` where v is the orbital speed of satellite then find maximum distance of satellite from the center of the earth.

A

`R_e`

B

`2R_e`

C

`3R_e`

D

`4R_e`

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The correct Answer is:
To solve the problem of finding the maximum distance of a satellite from the center of the Earth after its velocity is increased, we can follow these steps: ### Step-by-Step Solution: 1. **Identify Initial Conditions**: - The satellite is initially in a circular orbit at a radius \( R_e \) (the radius of the Earth). - The orbital speed \( v \) of the satellite at this radius is given by the formula: \[ v = \sqrt{\frac{GM}{R_e}} \] where \( G \) is the gravitational constant and \( M \) is the mass of the Earth. 2. **Increase Velocity**: - The velocity of the satellite is increased to \( v' = \sqrt{\frac{3}{2}} v \). 3. **Conservation of Energy**: - The total mechanical energy (kinetic + potential) is conserved when no external work is done. - The potential energy \( U \) at a distance \( r \) from the center of the Earth is given by: \[ U = -\frac{GMm}{r} \] - The kinetic energy \( K \) of the satellite is given by: \[ K = \frac{1}{2} mv'^2 \] 4. **Calculate Initial Energy**: - At the initial position (radius \( R_e \)): \[ U_1 = -\frac{GMm}{R_e} \] \[ K_1 = \frac{1}{2} m v^2 = \frac{1}{2} m \left(\frac{GM}{R_e}\right) = \frac{GMm}{2R_e} \] - Total energy at position 1: \[ E_1 = U_1 + K_1 = -\frac{GMm}{R_e} + \frac{GMm}{2R_e} = -\frac{GMm}{2R_e} \] 5. **Calculate Final Energy**: - At the maximum distance \( r \) from the center of the Earth: \[ U_2 = -\frac{GMm}{r} \] \[ K_2 = \frac{1}{2} m v'^2 = \frac{1}{2} m \left(\frac{3}{2} v\right)^2 = \frac{1}{2} m \left(\frac{3}{2}\right)^2 \left(\frac{GM}{R_e}\right) = \frac{9GMm}{8R_e} \] - Total energy at position 2: \[ E_2 = U_2 + K_2 = -\frac{GMm}{r} + \frac{9GMm}{8R_e} \] 6. **Set Energies Equal**: - Since energy is conserved: \[ E_1 = E_2 \] \[ -\frac{GMm}{2R_e} = -\frac{GMm}{r} + \frac{9GMm}{8R_e} \] 7. **Solve for \( r \)**: - Rearranging gives: \[ -\frac{GMm}{2R_e} + \frac{9GMm}{8R_e} = -\frac{GMm}{r} \] \[ \frac{9GMm}{8R_e} - \frac{4GMm}{8R_e} = -\frac{GMm}{r} \] \[ \frac{5GMm}{8R_e} = -\frac{GMm}{r} \] - Cross-multiplying gives: \[ 5r = -8R_e \implies r = \frac{8R_e}{5} \] 8. **Final Result**: - The maximum distance of the satellite from the center of the Earth is: \[ r = 2R_e \]
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