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Eccentric anomaly

The eccentric anomaly of point <i>p</i> is the angle <i>z-c-x</i>
The eccentric anomaly of point p is the angle z-c-x
In celestial mechanics, the eccentric anomaly is an angular parameter that defines the position of a body that is moving along an elliptic Kepler orbit.

For the point p=(x,y) on an ellipse with the equation
\frac{x^2}{a^2} + \frac{y^2}{b^2} = 1

the eccentric anomaly is the angle E such that
\cos E = \frac{x}{a}\quad \quad \sin E = \frac{y}{b}

The eccentric anomaly is one of three angular parameters ("anomalies") that define a position along an orbit; the other two being the true anomaly and the mean anomaly.

Formulas

From the true anomaly

The eccentric anomaly can be computed from the true anomaly by the formulas
\cos E = \frac{x}{a} = \frac{ e + \cos \theta }{1 + e \cos \theta }

\sin E = \frac{y}{b} = \frac{ \sqrt{1 - e^2} \, \sin \theta }{1 + e \cos \theta }

hence
E = \mathop{\mathrm{arg}}( e + \cos \theta, \; \sqrt{1 - e^2} \, \sin \theta)

where \mathop{\mathrm{arg}}(X,Y) is the angular coordinate of point (X,Y) in polar coordinates.

From the mean anomaly

The eccentric anomaly E is related to the mean anomaly M by the formula
M = E - e \cdot \sin E

This equation does not have a closed-form solution for E given M. It is usually solved by numerical methods, e.g. Newton-Raphson method.

Radius and eccentric anomaly

The radius (distance from the focus of attraction to the orbiting body) is related to the eccentric anomaly by the formula
r = a \left ( 1 - e \cdot \cos{E} \right )

 
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