Algebraic function: Difference between revisions

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In [[celestial mechanics]], the '''eccentricity vector''' of a [[Kepler orbit]] is the [[vector (geometric)|vector]] that points towards the [[periapsis]] and has a magnitude equal to the orbit's scalar [[orbital eccentricity|eccentricity]]. The magnitude is [[unitless]]. 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 orbit|osculating]] eccentricity vector to change continuously. For the eccentricity and [[argument of periapsis]] parameters, eccentricity zero (circular orbit) corresponds to a singularity.
 
==Calculation==
The '''eccentricity vector''' <math> \mathbf{e} \,</math> can be calculated<ref>{{cite book |title=The Kepler Problem |first=Bruno |last=Cordani |page=22 |location= |publisher=Birkhaeuser |year=2003 |isbn=3-7643-6902-7 }}</ref>
 
:<math> \mathbf{e} = {\mathbf{v}\times\mathbf{h}\over{\mu}} - {\mathbf{r}\over{\left|\mathbf{r}\right|}}</math>
where:
*<math> \mathbf{v}\,\!</math> is [[velocity vector]]
*<math>\mathbf{h}\,\!</math> is [[Specific relative angular momentum|specific angular momentum vector]] (equal to <math>\mathbf{r}\times\mathbf{v}</math>)
*<math>\mathbf{r}\,\!</math> is [[position vector]]
*<math>\mu\,\!</math> is [[standard gravitational parameter]]
 
or equivalently:
:<math> \mathbf{e} = {\mathbf{\left |v \right |}^2 \mathbf{r} \over {\mu}} - {(\mathbf{r} \cdot \mathbf{v} ) \mathbf{v} \over{\mu}} - {\mathbf{r}\over{\left|\mathbf{r}\right|}}</math>
 
==See also==
*[[Kepler orbit]]
*[[Orbit]]
*[[Eccentricity (orbit)|Eccentricity]]
*[[Laplace–Runge–Lenz vector]]
 
==References==
{{Reflist}}
 
{{DEFAULTSORT:Eccentricity Vector}}
[[Category:Orbits]]
[[Category:Vectors]]

Revision as of 18:50, 21 January 2014

In celestial mechanics, the eccentricity vector of a Kepler orbit is the vector that points towards the periapsis and has a magnitude equal to the orbit's scalar eccentricity. The magnitude is unitless. 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. For the eccentricity and argument of periapsis parameters, eccentricity zero (circular orbit) corresponds to a singularity.

Calculation

The eccentricity vector e can be calculated[1]

e=v×hμr|r|

where:

or equivalently:

e=|v|2rμ(rv)vμr|r|

See also

References

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