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 of the satellite is : |
\(\sqrt{\frac{gR}{R-x}}\) \(\sqrt{\frac{gR^2}{R-x}}\) \(\sqrt{gx}\) \(\sqrt{\frac{gR^2}{R+x}}\) |
\(\sqrt{\frac{gR^2}{R+x}}\) |
\(mg (1 + \frac{x}{R})^{-2} = \frac{mv^2}{R+x}\) \(\Rightarrow v = \sqrt{g(R+x)\frac{R^2}{(R+x)^2}}\) \(\Rightarrow v = \sqrt{\frac{gR^2}{R+x}}\)
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