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Question: A satellite is geostationary in a particular orbit. It is allowed to go to another orbit having an o...

A satellite is geostationary in a particular orbit. It is allowed to go to another orbit having an orbital radius 2 times that of the earlier orbit from the centre of the earth. The time period in the second orbit is
A. 48 hours
B. 24 hours
C. 482hours48\sqrt 2 \,{\text{hours}}
D. 242hours24\sqrt 2 \,{\text{hours}}

Explanation

Solution

Use Kepler’s third law to determine the orbital period of the satellite in the second orbit. For a geostationary satellite, the orbital period of the satellite in orbit is the same as the rotation period of the earth.

Formula used:
T2=4π2GMa3{T^2} = \dfrac{{4{\pi ^2}}}{{GM}}{a^3}
Here, G is the universal gravitational constant, M is the mass of earth and a is the semimajor axis of the orbit of satellite.

Complete step by step answer:
According to Kepler’s third law, the period of satellite moving in a orbit of semimajor axis a is given as,
T2=4π2GMa3{T^2} = \dfrac{{4{\pi ^2}}}{{GM}}{a^3}
Here, G is the universal gravitational constant, M is the mass of earth and a is the semimajor axis of the orbit of satellite.
For the first orbit, the period of the satellite in its orbit will be,
T12=4π2GMa13T_1^2 = \dfrac{{4{\pi ^2}}}{{GM}}a_1^3 …… (1)
For the second orbit, the period of the satellite in that orbit will be,
T22=4π2GMa23T_2^2 = \dfrac{{4{\pi ^2}}}{{GM}}a_2^3 …… (2)
Divide equation (2) by equation (1).
T22T12=4π2GMa234π2GMa13\dfrac{{T_2^2}}{{T_1^2}} = \dfrac{{\dfrac{{4{\pi ^2}}}{{GM}}a_2^3}}{{\dfrac{{4{\pi ^2}}}{{GM}}a_1^3}}
T22T12=(a2a1)3\Rightarrow \dfrac{{T_2^2}}{{T_1^2}} = {\left( {\dfrac{{{a_2}}}{{{a_1}}}} \right)^3}
T2=(a2a1)32T1\therefore {T_2} = {\left( {\dfrac{{{a_2}}}{{{a_1}}}} \right)^{\dfrac{3}{2}}}{T_1}
For a geostationary orbit, the orbital period is 24 hours.
We have given, the radius of the second orbit is twice of the first orbit. Therefore, substitute 2a12{a_1} for a2{a_2} and 24 hours for T1{T_1} in the above equation.
T2=(2a1a1)32(24hours){T_2} = {\left( {\dfrac{{2{a_1}}}{{{a_1}}}} \right)^{\dfrac{3}{2}}}\left( {24\,{\text{hours}}} \right)
T2=(2)32(24hours)\Rightarrow {T_2} = {\left( 2 \right)^{\dfrac{3}{2}}}\left( {24\,{\text{hours}}} \right)
T2=22(24hours)\Rightarrow {T_2} = 2\sqrt 2 \left( {24\,{\text{hours}}} \right)
T2=482 hours\therefore {T_2} = 48\sqrt 2 {\text{ hours}}

So, the correct answer is “Option C”.

Note:
As the radius of the orbit increases, the period of the satellite also increases.
To check whether your answer is right or wrong refer to the above conclusion.