Jump to content

Dermott's law: Difference between revisions

From Wikipedia, the free encyclopedia
Content deleted Content added
No edit summary
No edit summary
Line 5: Line 5:
where ''T(n)'' is the orbital period of the n<sup>th</sup> satellite, ''T(0)'' is of the order of days and ''C'' is a constant of the satellite system in question. Specific values are:
where ''T(n)'' is the orbital period of the n<sup>th</sup> satellite, ''T(0)'' is of the order of days and ''C'' is a constant of the satellite system in question. Specific values are:


*''[[Jovian system]]'': &nbsp;&nbsp;&nbsp; T(0) = 0.444 d, C = 2.03
*''[[Jovian system]]'': &nbsp;&nbsp;&nbsp; T(0) = 0.444 [[Day|d]], C = 2.03
*''[[Saturnian system]]'': T(0) = 0.462 d, C = 1.59
*''[[Saturnian system]]'': T(0) = 0.462 d, C = 1.59
*''[[Uranian system]]'': &nbsp;&nbsp; T(0) = 0.488 d, C = 2.24
*''[[Uranian system]]'': &nbsp;&nbsp; T(0) = 0.488 d, C = 2.24

Revision as of 09:32, 28 June 2010

Dermott's Law is an empirical formula for the orbital period of major satellites orbiting planets in the solar system. It was identified by the celestial mechanics researcher Stanley Dermott in the 1960s and takes the form:

where T(n) is the orbital period of the nth satellite, T(0) is of the order of days and C is a constant of the satellite system in question. Specific values are:

Such power-laws may be a consequence of collapsing-cloud models of planetary and satellite systems possessing various symmetries; see Titius-Bode Law. They may also reflect the effect of resonance-driven commensurabilities in the various systems.

References

  • "On the origin of commensurabilities in the solar system - II: the orbital period relation" S. F. Dermott, Mon. Not. RAS vol. 141 pp363-376 (1968).
  • "On the origin of commensurabilities in the solar system - III: the resonant structure of the solar system" S. F. Dermott, Mon. Not. RAS vol. 142 pp143-149 (1969).