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If a planet of radius R and density D is...

If a planet of radius R and density D is revolving around the sun in a circular orbit of radius r with time period T, then the mass of the sun is

A

`(4pi^2r^3)/(GT)`

B

`(4pi^2r^3)/(GT^2)`

C

`(4pi^2r)/(GT)`

D

`(4pi^2r^3)/(G^2T^2)`

Text Solution

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The correct Answer is:
To find the mass of the Sun (M) given a planet of radius R and density D revolving around it in a circular orbit of radius r with time period T, we can follow these steps: ### Step-by-Step Solution: 1. **Use Kepler's Third Law**: According to Kepler's Third Law, the square of the time period (T) of a planet is directly proportional to the cube of the radius (r) of its orbit around the Sun. This can be expressed mathematically as: \[ T^2 \propto r^3 \] This implies: \[ T^2 = k \cdot r^3 \] where k is a constant. 2. **Apply Newton's Law of Gravitation**: The gravitational force acting on the planet can be expressed using Newton's law of gravitation: \[ F = \frac{G \cdot M \cdot m}{r^2} \] where G is the gravitational constant, M is the mass of the Sun, and m is the mass of the planet. 3. **Centripetal Force**: For a planet moving in a circular orbit, the centripetal force required to keep it in that orbit is given by: \[ F = \frac{m v^2}{r} \] where v is the orbital velocity of the planet. 4. **Equate the Forces**: Since the gravitational force provides the necessary centripetal force, we can set the two expressions for force equal to each other: \[ \frac{m v^2}{r} = \frac{G \cdot M \cdot m}{r^2} \] We can cancel m from both sides (assuming m ≠ 0): \[ \frac{v^2}{r} = \frac{G \cdot M}{r^2} \] Rearranging gives: \[ v^2 = \frac{G \cdot M}{r} \] 5. **Relate Velocity to Time Period**: The velocity (v) of the planet can also be expressed in terms of the time period (T): \[ v = \frac{2 \pi r}{T} \] Squaring this gives: \[ v^2 = \left(\frac{2 \pi r}{T}\right)^2 = \frac{4 \pi^2 r^2}{T^2} \] 6. **Substitute into the Equation**: Now we can substitute this expression for \(v^2\) into the equation we derived from equating the forces: \[ \frac{4 \pi^2 r^2}{T^2} = \frac{G \cdot M}{r} \] 7. **Solve for Mass of the Sun (M)**: Rearranging this equation to solve for M gives: \[ M = \frac{4 \pi^2 r^3}{G T^2} \] ### Final Expression: Thus, the mass of the Sun (M) is given by: \[ M = \frac{4 \pi^2 r^3}{G T^2} \]
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