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Question: Let the kinetic energy of a satellite is \[x\], then its time of revolution \[T\] is proportional to...

Let the kinetic energy of a satellite is xx, then its time of revolution TT is proportional to
(A) x3{x^{ - 3}}
(B) x32{x^{ - \dfrac{3}{2}}}
(C) x1{x^{ - 1}}
(D) x\sqrt x

Explanation

Solution

We can recall that the period of revolution of an orbiting is the time taken to complete a cycle of its orbit. The centripetal force required to keep any object in orbit about a planet is provided by the gravitational force of attraction which pulls the object towards the planet
Formula used: In this solution we will be using the following formulae;
KE=12mv2KE = \dfrac{1}{2}m{v^2} where KEKE is the kinetic energy of a body, mm is the mass of the body, and vv is the velocity of the body.
R=GMv2R = \dfrac{{GM}}{{{v^2}}} where RR is the radius of an object orbiting a planet, GG is the universal gravitational constant, MM is the mass of the planet and vv is the velocity of the orbiting object at that specific radius.
T=2πRvT = \dfrac{{2\pi R}}{v} where TT is the period of revolution of the orbit.

Complete Step-by-Step solution:
To solve this we note that
KE=12mv2KE = \dfrac{1}{2}m{v^2} where KEKE is the kinetic energy of a body, mm is the mass of the body, and vv is the velocity of the body.
Hence, x=12mv2x = \dfrac{1}{2}m{v^2}
v=(2xm)12\Rightarrow v = {\left( {\dfrac{{2x}}{m}} \right)^{\dfrac{1}{2}}}
Now, recalling that the period can be defined as
T=2πRvT = \dfrac{{2\pi R}}{v} where TT is the period of revolution of the orbit, where RR is the radius of an object satellite the planet.
But the radius can be given as
R=GMv2R = \dfrac{{GM}}{{{v^2}}}
Hence, inserting into T=2πRvT = \dfrac{{2\pi R}}{v}
T=2π(GMv2)v=2GMπv3T = \dfrac{{2\pi \left( {\dfrac{{GM}}{{{v^2}}}} \right)}}{v} = \dfrac{{2GM\pi }}{{{v^3}}}
But v=(2xm)12v = {\left( {\dfrac{{2x}}{m}} \right)^{\dfrac{1}{2}}}
Hence,
T=2GMπ((2xm)12)3T = \dfrac{{2GM\pi }}{{{{\left( {{{\left( {\dfrac{{2x}}{m}} \right)}^{\dfrac{1}{2}}}} \right)}^3}}}
T2GMπm32832x32T \Rightarrow \dfrac{{2GM\pi {m^{\dfrac{3}{2}}}}}{{{8^{\dfrac{3}{2}}}{x^{\dfrac{3}{2}}}}}
Hence, is inversely proportional to x32{x^{\dfrac{3}{2}}} or proportional to x32{x^{ - \dfrac{3}{2}}}

Thus, the correct option is B

Note: For clarity, the formula for the radius of the orbiting object R=Gmv2R = \dfrac{{Gm}}{{{v^2}}} can be gotten from the knowledge that the centripetal force for revolution is provided by the gravitational force of attraction. Hence,
mv2R=GmMR2\dfrac{{m{v^2}}}{R} = \dfrac{{GmM}}{{{R^2}}} where all quantities take the value as specified previously.
Hence, by dividing both sides by mm and multiplying by RR, we have
v2=GMR{v^2} = \dfrac{{GM}}{R}
R=GMv2\Rightarrow R = \dfrac{{GM}}{{{v^2}}}