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In celestial mechanics, the eccentricity vector of a Kepler orbit is the dimensionless vector with direction pointing from apoapsis to periapsis and with magnitude equal to the orbit's scalar eccentricity. For Kepler orbits the eccentricity vector is a constant of motion. Its main use is in the analysis of almost circular orbits, as perturbing (non-Keplerian) forces on an actual orbit will cause the osculating eccentricity vector to change continuously as opposed to the eccentricity and argument of periapsis parameters for which eccentricity zero (circular orbit) corresponds to a singularity.

Calculation

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The eccentricity vector is: [1]

which follows immediately from the vector identity:

where:

See also

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References

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  1. ^ Cordani, Bruno (2003). The Kepler Problem. Birkhaeuser. p. 22. ISBN 3-7643-6902-7.

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Eccentricity (mathematics)

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developed. The eccentricity of an orbit can be calculated from the orbital state vectors as the magnitude of the eccentricity vector: e = | e | {\displaystyle

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current position of an object on its orbit Eccentricity vector, in celestial mechanics, a dimensionless vector with direction pointing from apoapsis to

Kepler orbit

direction of the periapsis of the orbit. We can then define the eccentricity vector associated with the orbit as: e ≜ c α = r ˙ × H α − u = v × H α −

Orbital station-keeping

Solar radiation pressure will in general perturb the eccentricity (i.e. the eccentricity vector); see Orbital perturbation analysis (spacecraft). For

Elliptic orbit

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Argument of periapsis

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