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The ratio of binding energy of a satel...

The ratio of binding energy of a satellite at rest on earth's surface to the binding energy of a satellite of same mass revolving around of the earth at a height h above the earth's surface is (R = radius of the earth).

A

`(2(R+h))/R`

B

`(R+h)/(2R)`

C

`(R+h)/R`

D

`R/(R+h)`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem of finding the ratio of the binding energy of a satellite at rest on the Earth's surface to the binding energy of a satellite of the same mass revolving around the Earth at a height \( h \) above the Earth's surface, we can follow these steps: ### Step 1: Understand the Binding Energy at Earth's Surface The binding energy \( E_1 \) of a satellite at rest on the Earth's surface can be expressed using the formula for gravitational potential energy. The binding energy is given by: \[ E_1 = -\frac{G M m}{R} \] where: - \( G \) is the gravitational constant, - \( M \) is the mass of the Earth, - \( m \) is the mass of the satellite, - \( R \) is the radius of the Earth. ### Step 2: Understand the Binding Energy of a Satellite in Orbit For a satellite revolving around the Earth at a height \( h \) above the Earth's surface, the distance from the center of the Earth is \( R + h \). The binding energy \( E_2 \) of this satellite can be expressed as: \[ E_2 = -\frac{G M m}{R + h} \] ### Step 3: Calculate the Ratio of Binding Energies We need to find the ratio of the binding energy at the Earth's surface to the binding energy of the satellite in orbit: \[ \text{Ratio} = \frac{E_1}{E_2} = \frac{-\frac{G M m}{R}}{-\frac{G M m}{R + h}} = \frac{R + h}{R} \] ### Step 4: Simplify the Ratio The ratio simplifies to: \[ \text{Ratio} = \frac{R + h}{R} = 1 + \frac{h}{R} \] ### Conclusion Thus, the final expression for the ratio of the binding energy of a satellite at rest on the Earth's surface to the binding energy of a satellite of the same mass revolving around the Earth at a height \( h \) is: \[ \text{Ratio} = 1 + \frac{h}{R} \]
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