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Question: The time period of an earth satellite in a circular orbit of radius \(R\) is \(2\) days and its orbi...

The time period of an earth satellite in a circular orbit of radius RR is 22 days and its orbital velocity is v0{{v}_{0}}.If time period of another satellite in a circular orbit is 16 days then
A. Its radius of orbit is 4R4R and orbital velocity is v0{{v}_{0}}.
B. Its radius of orbit is 4R4R and orbital velocity is v02\dfrac{{{v}_{0}}}{2}
C. Its radius of orbit is 2R2R and orbital velocity is v0{{v}_{0}}
D. Its radius of orbit is 2R2R and orbital velocity is v02\dfrac{{{v}_{0}}}{2}

Explanation

Solution

Kepler’s third law relates the time period of a planetary object with the radius of orbit. Using this Kepler’s third law calculates the radius of the orbit of the 2nd satellite. Using this radius calculate the orbital velocity of the satellite.

Formula used:
The square time period TT of a satellite is directly proportional to the cube of the radius RR of the orbit and is given by T2αR3{{T}^{2}}\alpha {{R}^{3}}.
For two different objects. Of time periods T1 and T2{{T}_{1}}\text{ and }{{T}_{2}} of radius R1 and R2{{R}_{1}}\text{ and }{{R}_{2}} it is given by
T12T22=R13R23\dfrac{{{T}_{1}}^{2}}{{{T}_{2}}^{2}}=\dfrac{R_{1}^{3}}{R_{2}^{3}}
The orbital velocity of the satellite of radius RRof time period TTis
v=(circumference of the orbittime period)v=\left( \dfrac{\text{circumference of the orbit}}{\text{time period}} \right)
So, v=2πRTv=\dfrac{2\pi R}{T}

Complete answer:
According to Kepler’s third law of planetary motion, the square of time period of revolution of any object around the sun or the earth is directly proportional to the cube of the radius i.e.
T2αR3{{T}^{2}}\alpha {{R}^{3}}
For two different objects. Of time periods T1 and T2{{T}_{1}}\text{ and }{{T}_{2}} of radius R1 and R2{{R}_{1}}\text{ and }{{R}_{2}} it is given by
T12T22=R13R23\dfrac{{{T}_{1}}^{2}}{{{T}_{2}}^{2}}=\dfrac{R_{1}^{3}}{R_{2}^{3}}
For the first satellite. R1=R{{R}_{1}}=R,T1=2 days{{T}_{1}}=2\text{ days}
For the second satellite. T2=16 days{{T}_{2}}=16\text{ days}
So
T12T22=R13R23 R23=T22T12R13 \begin{aligned} & \dfrac{{{T}_{1}}^{2}}{{{T}_{2}}^{2}}=\dfrac{R_{1}^{3}}{R_{2}^{3}} \\\ & \Rightarrow R_{2}^{3}=\dfrac{{{T}_{2}}^{2}}{{{T}_{1}}^{2}}R_{1}^{3} \\\ \end{aligned}
Putting the values of T1,T2 and R2{{T}_{1}},{{T}_{2}}\text{ and }{{R}_{2}}we get.
R23=(162)2R3=64R3 R2=64R33=4R \begin{aligned} & R_{2}^{3}={{\left( \dfrac{16}{2} \right)}^{2}}{{R}^{3}}=64{{R}^{3}} \\\ & \Rightarrow {{R}_{2}}=\sqrt[3]{64{{R}^{3}}}=4R \\\ \end{aligned}
So the radius of second satellite is 4R4R
Now the orbital velocity of this satellite is given by
v=(circumference of the orbittime period)=2πR2T2 v=2π(4R)16=2πR4=12v0 \begin{aligned} & v=\left( \dfrac{\text{circumference of the orbit}}{\text{time period}} \right)=\dfrac{2\pi {{R}_{2}}}{{{T}_{2}}} \\\ & \Rightarrow v=\dfrac{2\pi (4R)}{16}=\dfrac{2\pi R}{4}=\dfrac{1}{2}{{v}_{0}} \\\ \end{aligned}
Where v0=2πR2{{v}_{0}}=\dfrac{2\pi R}{2} is the orbital velocity of the first satellite.
So the radius of 2nd satellite is 4R4R and its orbital velocity will be v02\dfrac{{{v}_{0}}}{2}

So, the correct answer is “Option B”.

Additional Information:
Kepler’s first law: Each planet revolves around the sun in an elliptical orbit with the sun situated at one of its foci.
Kepler’s second law(law of areas): The area vector drawn from the sun to a planet sweeps out an equal area in an equal interval of time.
Kepler’s third law: the square of period of revolution of a planet around the sun is proportional to the cube of the semi major axis of its elliptical orbit.

Note:
Note that Kepler’s law is valid for any object revolving around any object. It is also valid for circular orbit. A planet revolves around the sun due to the centripetal force of the sun which is directed towards the sun. You can also calculate the angular momentum of revolution if you know orbital velocity and radius by the formula
L=mvrL=mvr