Difference between revisions of "Orbital eccentricity"

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(Math enhancement)
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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/a</math>
+
<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 ''e'' = 0.
+
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,
  
−
Therefore, for any closed orbit, <math>0 <= e <= 1</math>.
+
<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 = (Q + q)/2</math>
+
<math>a=\frac{Q + q}{2}</math>
  
−
<math>e = (Q - q)/(Q + q)</math>
+
<math>e=\frac{Q - q}{Q + q}</math>
  
 
or
 
or
  
−
<math>e = 1 - 2/((Q/q) + 1)</math>
+
<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 = (1+e)/(1-e)</math>
+
<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(1+e)/(1-e) = 0</math>
+
<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 + (1+e)/(1-e)) = 2a</math>
+
<math>q\left (1 + \frac{1+e}{1-e}\right ) = 2a</math>
  
 
From the above:
 
From the above:
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<math>Q = a(1+e)</math>
 
<math>Q = a(1+e)</math>
  
−
For ''e'' = 0, Q = q = a = r, the orbital radius, as one would expect.
+
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.