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).
Variables used in this article


Contents
Calculation
See also
References

Calculation


In astrodynamics eccentric anomaly ''E'' can be calculated as follows:
:E=rccos {{1-left | mathbf{r}
ight | / a} over e}
where:

mathbf{r},! is the orbiting body's position vector (segment ''sp''),

a,! is the orbit's semi-major axis (segment ''cz''), and

e,! is the orbit's eccentricity.
The relation between ''E'' and ''M'', the mean anomaly, is:
:M = E - e cdot sin{E}.,!
For small values of e (e < 0.6627434 ) this equation can be solved iteratively, starting from E_0 = M and using the relation E_{i+1} = M + e,sin E_i. The first few terms of the expansion in powers of e are:

E_1 = M + e,sin M

E_2 = M + e,sin M + rac{1}{2} e^2 sin 2M

E_3 = M + e,sin M + rac{1}{2} e^2 sin 2M
+ rac{1}{8} e^3 (3sin 3M - sin M).
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 ''T'', the true anomaly, is:
:cos{T} = {{cos{E} - e} over {1 - e cdot cos{E}}}
or equivalently
: an{T over 2} = sqrt{{{1+e} over {1-e}}} an{E over 2}.,
The relations between the radius (position vector magnitude) and the anomalies are:
:r = a left ( 1 - e cdot cos{E}
ight ),!
and
:r = a{(1 - e^2) over (1 + e cdot cos{T})}.,!

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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