(astronomy) An orbit comprising a complete constant-altitude revolution around the earth.
| Sci-Tech Dictionary: circular orbit |
(astronomy) An orbit comprising a complete constant-altitude revolution around the earth.
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| Wikipedia: Circular orbit |
In astrodynamics or celestial mechanics a circular orbit is an elliptic orbit with the eccentricity equal to 0. It is an example of a rotation around a fixed axis: this axis is the line through the center of mass perpendicular to the plane of motion.
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Transverse acceleration (perpendicular to velocity) causes change in direction. If it is constant in magnitude and changing in direction with the velocity, we get a circular motion. For this centripetal acceleration we have

where:
is orbital velocity of orbiting body,
is radius of the circle
is angular frequency, measured in radians per second.Under standard assumptions the orbital velocity of a body traveling along circular orbit,
can be computed as:

where:
is radius of orbit equal to radial distance of orbiting body from central body,
is the standard gravitational parameter, which is the product of the gravitational constant G and the central mass M.Conclusion:
Under standard assumptions the orbital period (
) of a body traveling along circular orbit can be computed as:

where:
is the semi-major axis of the orbit; radius of the central body plus altitude of the orbit
is standard gravitational parameter.Under standard assumptions, specific orbital energy (
) is negative for a closed orbit and the orbital energy conservation equation (the Vis-viva equation) can take the form:

where:
is orbital velocity of orbiting body,
is radius of orbit equal to radial distance of orbiting body from central body,
is standard gravitational parameter.The boundary case is
which corresponds to escape from the primary (parabolic orbit), with
.
The virial theorem applies even without taking a time-average:
Thus the escape velocity from any distance is √2 times the speed in a circular orbit at that distance: the kinetic energy is twice as much, hence the total energy is zero.
Under standard assumptions, the orbital equation becomes:

where:
is radial distance of orbiting body from central body,
is specific angular momentum of the orbiting body,
is standard gravitational parameter.Maneuvering into a large circular orbit, e.g. a geostationary orbit, requires a larger delta-v than an escape orbit, although the latter implies getting arbitrarily far away and having more energy than needed for the orbital speed of the circular orbit. It is also a matter of maneuvering into the orbit. See also Hohmann transfer orbit.
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