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Mean anomaly
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In celestial mechanics, mean anomaly is one of the orbital elements that defines a Kepler orbit. It specifies the position of the orbiting objects along the ellipse defined by the other elements, but does not correspond to an actual geometric angle. True anomaly specifies the real geometric angle between periapsis (closest approach to the central body) and the position of the orbiting body at any given time. Mean anomaly is similar, but unlike the real position of the orbiting body, always varies linearly with time (which is more mathematically convenient).
In the two-body problem for the case corresponding to an elliptic Kepler orbit, the relation between the Eccentric anomaly and the time is:
(1)
where is the eccentricity and is time counted from a pericentre passage.

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In celestial mechanics, mean anomaly is one of the orbital elements that defines a Kepler orbit. It specifies the position of the orbiting objects along the ellipse defined by the other elements, but does not correspond to an actual geometric angle. True anomaly specifies the real geometric angle between periapsis (closest approach to the central body) and the position of the orbiting body at any given time. Mean anomaly is similar, but unlike the real position of the orbiting body, always varies linearly with time (which is more mathematically convenient).
In the two-body problem for the case corresponding to an elliptic Kepler orbit, the relation between the Eccentric anomaly and the time is:
(1)
where is the eccentricity and is time counted from a pericentre passage. The mean anomaly is then defined as:
(2)
This fictive "angle" without direct geometrical meaning increases uniformly with time:
(3)
To find the position of the object in an elliptic Kepler orbit at a certain time, the corresponding mean anomaly is determined with (3) and then the corresponding Eccentric anomaly is found from (2) using the Newton-Raphson algorithm.
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