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III. Long Answer Questions · Q11

Q.Derive the time period of a satellite orbiting the Earth.

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Step 1. For a satellite of mass MsM_s in a circular orbit of radius (Re+h)(R_e+h), the gravitational force provides exactly the centripetal force needed:

Msv2Re+h=GMsMe(Re+h)2.\frac{M_sv^2}{R_e+h}=\frac{GM_sM_e}{(R_e+h)^2}.

Step 2. Cancelling MsM_s and one factor of (Re+h)(R_e+h): v2=GMeRe+h⇒v=GMeRe+hv^2=\dfrac{GM_e}{R_e+h}\Rightarrow v=\sqrt{\dfrac{GM_e}{R_e+h}}.

Step 3. The satellite covers the full circumference 2π(Re+h)2\pi(R_e+h) in one period TT, so v=2π(Re+h)Tv=\dfrac{2\pi(R_e+h)}{T}.

Step 4. Solving for TT: T=2π(Re+h)v=2π(Re+h)Re+hGMe=2π(Re+h)3GMeT=\dfrac{2\pi(R_e+h)}{v}=2\pi(R_e+h)\sqrt{\dfrac{R_e+h}{GM_e}}=2\pi\sqrt{\dfrac{(R_e+h)^3}{GM_e}}.

Step 5. For a satellite orbiting very close to the surface (h≪Reh\ll R_e, so Re+h≈ReR_e+h\approx R_e), using GMe=gRe2GM_e=gR_e^2: T=2πRe3gRe2=2πRegT=2\pi\sqrt{\dfrac{R_e^3}{gR_e^2}}=2\pi\sqrt{\dfrac{R_e}{g}}. …

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