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Eccentric anomaly

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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.

Contents

[edit] Formulas

[edit] 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.

[edit] 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.

[edit] 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 )

[edit] 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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