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Mean motion
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===Mean motion and the gravitational constants=== Two gravitational constants are commonly used in [[Solar System]] celestial mechanics: ''G'', the [[Gravitational constant|Newtonian constant of gravitation]] and ''k'', the [[Gaussian gravitational constant]]. From the above definitions, mean motion is :<math>n = \sqrt{\frac{ G( M + m ) }{a^3}}\,\!.</math> By normalizing parts of this equation and making some assumptions, it can be simplified, revealing the relation between the mean motion and the constants. Setting the mass of the [[Sun]] to unity, ''M'' = 1. The masses of the planets are all much smaller, {{nowrap|''m'' βͺ ''M''}}. Therefore, for any particular planet, :<math>n \approx \sqrt{\frac{G}{a^3}},</math> and also taking the semi-major axis as one [[astronomical unit]], :<math>n_{1\;\text{AU}} \approx \sqrt{G}.</math> The Gaussian gravitational constant ''k'' = {{sqrt|''G''}},<ref>{{cite book | last1 = U.S. Naval Observatory | first1=Nautical Almanac Office | last2 = H.M. Nautical Almanac Office | title = Explanatory Supplement to the Astronomical Ephemeris and the American Ephemeris and Nautical Almanac | publisher = H.M. Stationery Office, London | year = 1961 | page = 493 }}</ref><ref>{{cite book | last = Smart | first = W. M. | title = Celestial Mechanics | publisher = Longmans, Green and Co., London | year = 1953 | page=4 }}</ref><ref group=note>The [[Gaussian gravitational constant]], ''k'', usually has units of radians per day and the [[Gravitational constant|Newtonian constant of gravitation]], ''G'', is usually given in [[International System of Units|SI units]]. Be careful when converting.</ref> therefore, under the same conditions as above, for any particular planet :<math>n \approx \frac{k}{\sqrt{a^3}},</math> and again taking the semi-major axis as one astronomical unit, :<math>n_{1\text{ AU}} \approx k.</math>
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