Difference between revisions of "Orbital eccentricity"
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For the general case of an [[ellipse]] having semi-major axis a and distance c from the center to either focus: | For the general case of an [[ellipse]] having semi-major axis a and distance c from the center to either focus: | ||
| − | <math>e = c | + | <math>e=\frac{c}{a}</math> |
| − | A [[circle]] is a "degenerate" ellipse. In a circle, the two foci converge at the center. Therefore c = 0 and | + | A [[circle]] is a "degenerate" ellipse. In a circle, the two foci converge at the center. Therefore |
| + | |||
| + | <math>\mathrm{c} = 0</math> | ||
| + | |||
| + | and | ||
| + | |||
| + | <math>\mathit{e} = 0</math>. | ||
A [[parabola]] is an extreme case of an ellipse and is the first open conic section. For any parabola: | A [[parabola]] is an extreme case of an ellipse and is the first open conic section. For any parabola: | ||
| − | <math>e = 1</math> | + | <math>\mathit{e}=1</math> |
| + | |||
| + | Therefore, for any closed orbit, | ||
| − | + | <math>0 \le e \le 1</math> | |
== Practical application == | == Practical application == | ||
In astrodynamics, any given pair of [[apsis|apsides]] can predict the [[semi-major axis]] and eccentricity of any orbit. Specifically, for periapsis q and apoapsis Q: | In astrodynamics, any given pair of [[apsis|apsides]] can predict the [[semi-major axis]] and eccentricity of any orbit. Specifically, for periapsis q and apoapsis Q: | ||
| − | <math>a = | + | <math>a=\frac{Q + q}{2}</math> |
| − | <math>e = | + | <math>e=\frac{Q - q}{Q + q}</math> |
or | or | ||
| − | <math>e = 1 - 2 | + | <math>e = 1 - \frac{2}{(Q/q) + 1}</math> |
By the same token, a and ''e'' can predict Q and q. | By the same token, a and ''e'' can predict Q and q. | ||
| − | <math>Q/q = | + | <math>Q/q = \frac{1+e}{1-e}</math> |
and | and | ||
| − | <math>Q + q = 2a</math> | + | <math>\mathit{Q} + \mathit{q} = \mathit{2a}</math> |
Therefore | Therefore | ||
| − | <math>Q - q | + | <math>Q - q\frac{1+e}{1-e} = 0</math> |
and | and | ||
| − | <math>Q + q = 2a</math> | + | <math>\mathit{Q} + \mathit{q} = \mathit{2a}</math> |
Subtracting the first equation from the second yields | Subtracting the first equation from the second yields | ||
| − | <math>q(1 + | + | <math>q\left (1 + \frac{1+e}{1-e}\right ) = 2a</math> |
From the above: | From the above: | ||
| Line 55: | Line 63: | ||
<math>Q = a(1+e)</math> | <math>Q = a(1+e)</math> | ||
| − | For | + | For <math>\mathit{e} = 0</math>, <math>\mathit{Q} = \mathit{q} = \mathit{a} = \mathit{r}</math>, the orbital radius, as one would expect. |
[[Category:Astronomy]] | [[Category:Astronomy]] | ||
Revision as of 22:50, February 25, 2008
Orbital eccentricity is the measure of the departure of an orbit from a perfect circle.
Definitions
In geometry, eccentricity (e) is a concept universally applicable to conic sections.
For the general case of an ellipse having semi-major axis a and distance c from the center to either focus:
A circle is a "degenerate" ellipse. In a circle, the two foci converge at the center. Therefore
and
.
A parabola is an extreme case of an ellipse and is the first open conic section. For any parabola:
Therefore, for any closed orbit,
Practical application
In astrodynamics, any given pair of apsides can predict the semi-major axis and eccentricity of any orbit. Specifically, for periapsis q and apoapsis Q:
or
By the same token, a and e can predict Q and q.
and
Therefore
and
Subtracting the first equation from the second yields
From the above:
and
For , , the orbital radius, as one would expect.