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Two satellites of earth S(1) and S(2) ar...

Two satellites of earth `S_(1)` and `S_(2)` are moving in the same orbit. The mass of `S_(1)` is four times the mass of `S_(2)`. Which one of the following statements is true?

A

The potential energies of earth and satellite in the two cases are equal .

B

`S_(1)` and `S_(2)` are moving with the same speed.

C

The kinetic energies of the two satellites are equal .

D

The time period of `S_(1)` is four times that `S_(2)`.

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To solve the problem, we need to analyze the situation of two satellites, \( S_1 \) and \( S_2 \), moving in the same orbit around the Earth. The mass of satellite \( S_1 \) is four times the mass of satellite \( S_2 \). Let's denote the mass of \( S_2 \) as \( m \) and the mass of \( S_1 \) as \( 4m \). ### Step 1: Understand the gravitational force acting on the satellites The gravitational force \( F \) acting on a satellite in orbit is given by the formula: \[ F = \frac{G M m}{r^2} \] where \( G \) is the gravitational constant, \( M \) is the mass of the Earth, \( m \) is the mass of the satellite, and \( r \) is the distance from the center of the Earth to the satellite. ### Step 2: Apply the centripetal force condition For a satellite in circular motion, the gravitational force provides the necessary centripetal force: \[ \frac{G M m}{r^2} = \frac{m v^2}{r} \] where \( v \) is the orbital velocity of the satellite. ### Step 3: Derive the expression for orbital velocity From the equation above, we can simplify to find the orbital velocity \( v \): \[ v^2 = \frac{G M}{r} \] Thus, the orbital velocity \( v \) is given by: \[ v = \sqrt{\frac{G M}{r}} \] This shows that the orbital velocity depends only on the mass of the Earth \( M \) and the radius \( r \), and not on the mass of the satellite. ### Step 4: Analyze the kinetic energy of the satellites The kinetic energy \( KE \) of a satellite is given by: \[ KE = \frac{1}{2} m v^2 \] Substituting the expression for \( v^2 \): \[ KE = \frac{1}{2} m \left(\frac{G M}{r}\right) \] For satellite \( S_1 \) (mass \( 4m \)): \[ KE_{S_1} = \frac{1}{2} (4m) \left(\frac{G M}{r}\right) = 2m \left(\frac{G M}{r}\right) \] For satellite \( S_2 \) (mass \( m \)): \[ KE_{S_2} = \frac{1}{2} m \left(\frac{G M}{r}\right) = \frac{1}{2} m \left(\frac{G M}{r}\right) \] Thus, the kinetic energy of \( S_1 \) is four times that of \( S_2 \). ### Step 5: Analyze the gravitational potential energy The gravitational potential energy \( U \) of a satellite is given by: \[ U = -\frac{G M m}{r} \] For satellite \( S_1 \): \[ U_{S_1} = -\frac{G M (4m)}{r} = -\frac{4G M m}{r} \] For satellite \( S_2 \): \[ U_{S_2} = -\frac{G M m}{r} \] Thus, the gravitational potential energy of \( S_1 \) is four times that of \( S_2 \). ### Step 6: Analyze the time period of the satellites The time period \( T \) of a satellite in orbit is given by: \[ T = 2\pi \sqrt{\frac{r^3}{G M}} \] This expression shows that the time period depends only on the radius \( r \) and the mass of the Earth \( M \), and is independent of the mass of the satellite. ### Conclusion Based on the analysis: - The potential energy of \( S_1 \) is four times that of \( S_2 \). - The kinetic energy of \( S_1 \) is four times that of \( S_2 \). - The time period of both satellites is the same. Thus, the correct statement is that the time period of both satellites is the same. ### Final Answer The true statement is that both satellites have the same time period. ---

To solve the problem, we need to analyze the situation of two satellites, \( S_1 \) and \( S_2 \), moving in the same orbit around the Earth. The mass of satellite \( S_1 \) is four times the mass of satellite \( S_2 \). Let's denote the mass of \( S_2 \) as \( m \) and the mass of \( S_1 \) as \( 4m \). ### Step 1: Understand the gravitational force acting on the satellites The gravitational force \( F \) acting on a satellite in orbit is given by the formula: \[ F = \frac{G M m}{r^2} \] where \( G \) is the gravitational constant, \( M \) is the mass of the Earth, \( m \) is the mass of the satellite, and \( r \) is the distance from the center of the Earth to the satellite. ...
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