Time Period of Satellite — Core Principles
Core Principles
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 () and the orbital radius (). The fundamental formula is , where is the universal gravitational constant.
This shows that , 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.
Important Differences
vs Orbital Velocity
| Aspect | This Topic | Orbital Velocity |
|---|---|---|
| Definition | Time taken to complete one full revolution around the central body. | The tangential speed required to maintain a stable orbit at a given radius. |
| Formula | $T = 2pi \sqrt{\frac{r^3}{GM}}$ | $v = \sqrt{\frac{GM}{r}}$ |
| Dependency on Orbital Radius ($r$) | Increases with increasing $r$ ($T \propto r^{3/2}$). | Decreases with increasing $r$ ($v \propto 1/\sqrt{r}$). |
| Dependency on Satellite Mass ($m$) | Independent of satellite mass. | Independent of satellite mass. |
| Units | Seconds (s) | Meters per second (m/s) |
| Relationship | Related to orbital velocity by $T = \frac{2\pi r}{v}$. | Related to time period by $v = \frac{2\pi r}{T}$. |