Time Period of Satellite

Physics
NEET UG
Version 1Updated 24 Mar 2026

The time period of a satellite is defined as the total time taken by the satellite to complete one full revolution around its central celestial body, typically a planet like Earth. This orbital period is a crucial parameter in orbital mechanics, directly influenced by the mass of the central body and the radius of the satellite's orbit. It is fundamentally governed by the balance between the gravi…

Quick Summary

The time period of a satellite is the duration it takes to complete one full orbit around its central body. This period is governed by the balance between the gravitational force pulling the satellite towards the central body and the centripetal force required to maintain its circular path.

Crucially, the satellite's own mass does not influence its time period. Instead, it depends on the mass of the central body (MM) and the orbital radius (rr). The fundamental formula is T=2pisqrtr3GMT = 2pi sqrt{\frac{r^3}{GM}}, where GG is the universal gravitational constant.

This shows that T2proptor3T^2 propto r^3, a direct consequence of Kepler's Third Law. Satellites in higher orbits have longer time periods and slower orbital velocities. A special case is the geostationary satellite, which has a 24-hour time period and orbits at a specific radius, appearing stationary from Earth's surface, vital for communication and broadcasting.

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Key Concepts

Orbital Radius (rr)

The orbital radius is the distance from the center of the primary body (e.g., Earth) to the center of the…

Orbital Velocity (vv)

Orbital velocity is the speed at which a satellite travels along its orbit. It's the precise speed required…

Kepler's Third Law (T2proptor3T^2 propto r^3)

Kepler's Third Law, also known as the Law of Periods, states that for any satellite orbiting a central body,…

  • Definition:Time for one complete orbit.
  • Formula:T=2πr3GMT = 2\pi \sqrt{\frac{r^3}{GM}}
  • Orbital Radius:r=RE+hr = R_E + h
  • Dependencies:

- T2r3T^2 \propto r^3 (Kepler's Third Law) - T1/MT \propto 1/\sqrt{M}

  • Independence:TT is independent of satellite's mass (mm).
  • Geostationary Satellite:T=24,hoursT = 24,\text{hours}, fixed position relative to Earth's surface.

Three Radii Get Massive Time: T2r3/GMT^2 \propto r^3 / GM. (Helps remember T2T^2 is proportional to r3r^3 and inversely to GMGM). Also, Mass of Satellite Not Important (MSNI) for period.

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