Difference between revisions of "Eccentricity"
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− | + | Orbital '''eccentricity''' is the measure of the shape of a Kepler orbit, . | |
+ | |||
+ | Every orbit is a Kepler orbit in a two-body problem, taking the shape of a conic section. | ||
+ | Eccentricity of an orbit may be any non-negative value and is a dimensionless quantity, indicated by the variable e. | ||
+ | |||
+ | The eccentricity may take values as follows: | ||
+ | *Circular orbit e = 0 | ||
+ | *Elliptical orbit 0 < e < 1 | ||
+ | *Parabolic trajectory e = 1 | ||
+ | *Hyperbolic trajectory e > 1 | ||
+ | |||
+ | |||
+ | == See also == | ||
+ | [[w:Orbital eccentricity|Orbital eccentricity]] at Wikipedia. | ||
{{Stub}} | {{Stub}} | ||
+ | [[Category: Articles]] | ||
[[Category:Celestial mechanics]] | [[Category:Celestial mechanics]] |
Latest revision as of 03:46, 14 October 2022
Orbital eccentricity is the measure of the shape of a Kepler orbit, .
Every orbit is a Kepler orbit in a two-body problem, taking the shape of a conic section. Eccentricity of an orbit may be any non-negative value and is a dimensionless quantity, indicated by the variable e.
The eccentricity may take values as follows:
- Circular orbit e = 0
- Elliptical orbit 0 < e < 1
- Parabolic trajectory e = 1
- Hyperbolic trajectory e > 1
See also[edit]
Orbital eccentricity at Wikipedia.