MHT CET · Physics · Gravitation
The radius of the orbit of a geostationary satellite is (mean radius of the earth is \(\mathrm{R}\),
angular velocity about an axis in \(\omega\) and accleration due to gravity on earth's surface
is g)
- A \(\left(\frac{g R^{2}}{\omega^{2}}\right)^{1 / 3}\)
- B \(\frac{g R^{2}}{\omega^{2}}\)
- C \(\left(\frac{g R^{2}}{\omega^{2}}\right)^{2 / 3}\)
- D \(\left(\frac{g R^{2}}{\omega^{2}}\right)^{1 / 2}\)
Answer & Solution
Correct Answer
(A) \(\left(\frac{g R^{2}}{\omega^{2}}\right)^{1 / 3}\)
Step-by-step Solution
Detailed explanation
\(\begin{aligned} m r \omega^{2} &=\frac{G M m}{r^{2}} \\ r \omega^{2} &=\frac{G M}{r^{2}} \\ r^{3} &=\frac{G M}{\omega^{2}}=\frac{G M}{R^{2}} \times \frac{R^{2}}{\omega^{2}}=g \frac{R^{2}}{\omega^{2}} \\ r &=\left(\frac{R^{2} g}{\omega^{2}}\right)^{1 / 3} \end{aligned}\)
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