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Question: A satellite is in a circular orbit around a planet, its period of revolution is \(T\), radius of the...

A satellite is in a circular orbit around a planet, its period of revolution is TT, radius of the orbit is RR, orbital velocity VV and acceleration aa then:
A. V=aTV = aT and a=V2Ra = \dfrac{{{V^2}}}{R}
B. V=2πRTV = \dfrac{{2\pi R}}{T} and aTaT
C. V=2πRTV = \dfrac{{2\pi R}}{T} and a=V2Ra = \dfrac{{{V^2}}}{R}
D. V=12aT2V = \dfrac{1}{2}a{T^2}

Explanation

Solution

Recall the formula of centripetal acceleration and linear velocity. Find the relation between angular velocity and linear velocity to find the formula of linear velocity in terms of time period.

Complete step by step answer: Consider a satellite performing circular motion such that
RR is the radius
TT is the period of revolution
VV is linear or tangential velocity
aa is acceleration.
Then we know that acceleration always acts along the radius of the circular orbit. And it is called centripetal acceleration.
Centripetal acceleration is given by the formula,
a=V2Ra = \dfrac{{{V^2}}}{R}
The period of revolution is the time taken to complete one revolution.
It is given by
T=2πωT = \dfrac{{2\pi }}{\omega }
Where,
ω\omega is the angular velocity of the satellite
Rearranging it we can write
ω=2πT\omega = \dfrac{{2\pi }}{T}
But we also know that linear velocity is the product of angular velocity and radius of the orbit.
V=Rω\Rightarrow V = R\omega
V=2πRT\Rightarrow V = \dfrac{{2\pi R}}{T}
Thus the centripetal acceleration is a=V2Ra = \dfrac{{{V^2}}}{R} and linear velocity is V=2πRTV = \dfrac{{2\pi R}}{T}
Therefore, from the above explanation, the correct answer is, option (B) V=2πRTV = \dfrac{{2\pi R}}{T} and a=V2Ra = \dfrac{{{V^2}}}{R}

Note: To solve this question, you need to know the formulas used in rotational motion and the relation between angular and linear quantities like velocity etc.
Linear acceleration always acts along the center of the circle in which the body is orbiting and is also called the centripetal or radial acceleration.
Linear velocity always acts along the tangent to the circle in which the object is moving.