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A satellite of mass m is orbiting the earth in a circular orbit at a height 2R abvoe earth surface where R is the radius of the earth. If it starts losing energy at a constant rate `beta`, then it will fall on the earth surface after the time `t=(GMm)/(nbetaR)`. Assuming that the satellite is approximately in a circular orbit at all times, find the value of n.

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To solve the problem, we need to analyze the energy changes of a satellite in a circular orbit around the Earth as it loses energy at a constant rate and eventually falls to the Earth's surface. ### Step-by-Step Solution: 1. **Understanding the Initial and Final Conditions:** - The satellite is at a height of \(2R\) above the Earth's surface. Therefore, the distance from the center of the Earth is \(3R\) (since the radius of the Earth is \(R\)). - The satellite will eventually fall to the Earth's surface, which is at a distance of \(R\) from the center of the Earth. 2. **Total Energy of the Satellite:** - The total mechanical energy \(E\) of a satellite in orbit is given by: \[ E = -\frac{GMm}{2r} \] - For the initial position (at \(3R\)): \[ E_i = -\frac{GMm}{2 \times 3R} = -\frac{GMm}{6R} \] - For the final position (at \(R\)): \[ E_f = -\frac{GMm}{2R} \] 3. **Change in Energy:** - The change in energy as the satellite falls from its initial position to the final position can be expressed as: \[ E_f - E_i = -\frac{GMm}{2R} - \left(-\frac{GMm}{6R}\right) \] - Simplifying this: \[ E_f - E_i = -\frac{GMm}{2R} + \frac{GMm}{6R} = -\frac{3GMm}{6R} + \frac{GMm}{6R} = -\frac{2GMm}{6R} = -\frac{GMm}{3R} \] 4. **Rate of Energy Loss:** - The rate of energy loss is given as \(-\beta\). Therefore, we can write: \[ \frac{dE}{dt} = -\beta \] - This implies: \[ dE = -\beta dt \] 5. **Integrating the Energy Change:** - Integrating from the initial energy \(E_i\) to the final energy \(E_f\): \[ E_f - E_i = -\beta t \] - Substituting the change in energy: \[ -\frac{GMm}{3R} = -\beta t \] - Rearranging gives: \[ t = \frac{GMm}{3\beta R} \] 6. **Comparing with Given Time Expression:** - The problem states that the time \(t\) can also be expressed as: \[ t = \frac{GMm}{n\beta R} \] - By comparing both expressions for \(t\): \[ \frac{GMm}{3\beta R} = \frac{GMm}{n\beta R} \] - This leads to: \[ n = 3 \] ### Final Answer: Thus, the value of \(n\) is \(3\).
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