Q. A satellite of mass $m$ revolves around the earth of radius $R$ at a height $x$ from its surface. If $g\ $is the acceleration due to gravity on the surface of the earth, the orbital speed the satellite is

A) $gx$
B) $\frac{gR}{R - x}$
C) $\frac{{gR}^{2}}{R + x}$
D) $\left( \frac{{gR}^{2}}{R + x} \right)^{1/2}$
Explanation

(d) The gravitational force exerted on satellite at a height $x$ is
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ F_{G} = \frac{GM_{e}m}{(R + x)^{2}}$
where $M_{e} = mass\ of\ earth.$
Since, gravitational force provides the necessary centripetal force, so,
$\ \ \ \ \ \ \frac{GM_{e}m}{(R + x)^{2}} = \frac{mv_{o}^{2}}{(R + x)}$
where $v_{o}$ is orbital speed of satellite.
$\Longrightarrow \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \frac{GM_{e}m}{(R + x)} = mv_{o}^{2}$
$\Longrightarrow \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \frac{gR^{2}m}{(R + x)} = mv_{o}^{2}\ \ \ \ \ \ \ \ \ \left( \therefore g = \frac{GM_{e}}{R^{2}} \right)$
$\Longrightarrow \ \ v_{o} = \sqrt{\left\lbrack \frac{gR^{2}}{(R + x)} \right\rbrack} = \left\lbrack \frac{gR^{2}}{(R + x)} \right\rbrack^{1/2}$

Dr. Abubacker
Reviewed by Dr. Abubacker

Physics Educator & NEET/JEE Specialist

Ph.D. in Physics with 19+ years of teaching experience.

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