Satellites in orbit: mechanics and applications
Circular orbit of a satellite: speed, period, energy
Setting up the equation
A satellite of mass m in a circular orbit of radius r around a planet of mass M is subject only to the gravitational force, which acts as the centripetal force: GMm/r^2 = m*v^2/r
Orbital speed
From this we deduce the circular speed: v = sqrt(G*M/r)
The closer the satellite is to the planet, the greater its speed. Counter-intuitive result: raising a satellite to a higher orbit slows it down.
Orbital period
T = 2pir/v = 2pisqrt(r^3/(G*M))
Mechanical energy
Kinetic energy: Ec = (1/2)mv^2 = GMm/(2r) Gravitational potential energy (zero reference at infinity): Ep = -GMm/r Total mechanical energy: Em = Ec + Ep = -GMm/(2r)
Em is negative: the satellite is in a bound state. A positive or zero mechanical energy would correspond to an escape trajectory (hyperbola or parabola, not closed).
Table of quantities
| Quantity | Expression |
|---|---|
| Speed | v = sqrt(G*M/r) |
| Period | T = 2pisqrt(r^3/(G*M)) |
| Mechanical energy | Em = -GMm/(2*r) |
Classic pitfall
Do not confuse Ec and Em: we have Ec = -Em (and not Ec = Em). This is a direct consequence of the virial theorem for a 1/r potential, and a frequent source of sign errors in energy calculations.

