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| | {{Unreferenced stub|auto=yes|date=December 2009}} |
| | A '''Gaussian year''' is defined as 365.2568983 [[day]]s. It was adopted by [[Carl Friedrich Gauss]] as the length of the [[sidereal year]] in his studies of the dynamics of the solar system. |
| | A slightly different value is now accepted as the length of the sidereal year, |
| | and the value accepted by Gauss is given a special name. |
| | |
| | A particle of negligible mass, that orbits a body of 1 solar mass in this period, has a mean axis for its orbit of 1 [[astronomical unit]] by definition. The value is derived from [[Kepler's laws of planetary motion|Kepler's third law]] as |
| | |
| | :<math>\mbox{1 Gaussian year}= \frac {2\pi} {k} \,</math> |
| | |
| | where |
| | |
| | :''k'' is the [[Gaussian gravitational constant]]. |
| | |
| | ==See also== |
| | * [[Astronomical unit]] |
| | |
| | {{DEFAULTSORT:Gaussian Year}} |
| | <!-- [[Category:Astronomy]] too general --> |
| | [[Category:Units of time]] |
| | [[Category:Celestial coordinate system]] |
| | |
| | {{Astronomy-stub}} |
Revision as of 10:05, 9 November 2013
Template:Unreferenced stub
A Gaussian year is defined as 365.2568983 days. It was adopted by Carl Friedrich Gauss as the length of the sidereal year in his studies of the dynamics of the solar system.
A slightly different value is now accepted as the length of the sidereal year,
and the value accepted by Gauss is given a special name.
A particle of negligible mass, that orbits a body of 1 solar mass in this period, has a mean axis for its orbit of 1 astronomical unit by definition. The value is derived from Kepler's third law as
where
- k is the Gaussian gravitational constant.
See also
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