Eccentric anomaly
The eccentric anomaly is the angle between the direction of periapsis and the current position of an object on its orbit, projected onto the ellipse's circumscribing circle perpendicularly to the major axis, measured at the centre of the ellipse. In the diagram below, it is E (the angle zcx).
Calculation
In astrodynamics eccentric anomaly E can be calculated as follows:
where:
is the orbiting body's position vector (segment sp),
is the orbit's semi-major axis (segment cz), and
is the orbit's eccentricity.
The relation between E and M, the mean anomaly, is:
This equation can be solved iteratively, starting from E0 = M and using the relation
.
The equation can also be expanded in powers of e, as long as e < 0.6627434. The first few terms of the expansion are:
.
For references on details of this derivation, as well as other more efficient methods of solution, see Murray and Dermott (1999, p.35). For a derivation of the limiting value of e see Plummer (1960, section 46).
The relation between E and ν, the true anomaly, is:
or equivalently
The relations between the radius (position vector magnitude) and the anomalies are:
and
See also
- Kepler's laws of planetary motion
- Mean anomaly
- True anomaly
References
- Murray, C. D. & Dermott, S. F. 1999, Solar System Dynamics, Cambridge University Press, Cambridge.
- Plummer, H.C., 1960, An Introductory treatise on Dynamical Astronomy, Dover Publications, New York. (Reprint of the 1918 Cambridge University Press edition.)
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Source: adapted by the editor from Wikipedia, the free encyclopedia; from the article "Eccentric anomaly". Image Credit.
Inclination
Longitude of the ascending node
Argument of periapsis
Mean anomaly at epoch
True anomaly
Semi-minor axis
Linear eccentricity
Eccentric anomaly
Mean longitude
True longitude
Orbital period