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{| class="infobox bordered" style="font-size: 100%" cellpadding=3 | |||
|- | |||
! Body | |||
! ''μ'' (km<sup>3</sup>s<sup>−2</sup>) | |||
|- | |||
| [[Sun]] | |||
| {{val|132712440018|(9)}}<ref name="Astrodynamic Constants" /> | |||
|- | |||
| [[Mercury (planet)|Mercury]] | |||
| {{val|22032}} | |||
|- | |||
| [[Venus]] | |||
| {{val|324859}} | |||
|- | |||
| [[Earth]] | |||
| {{val|398600.4418|(9)}} | |||
|- | |||
| [[Moon]] | |||
| {{val|4902.8000}} | |||
|- | |||
| [[Mars]] | |||
| {{val|42828}} | |||
|- | |||
| [[1 Ceres|Ceres]] | |||
| {{val|63.1|(3)}}<ref name="Pitjeva2005" /><ref name="Britt2002" /> | |||
|- | |||
| [[Jupiter]] | |||
| {{val|126686534}} | |||
|- | |||
| [[Saturn]] | |||
| {{val|37931187}} | |||
|- | |||
| [[Uranus]] | |||
| {{val|5793939|(13)}}<ref name="Jacobson1992" /> | |||
|- | |||
| [[Neptune]] | |||
| {{val|6836529}} | |||
|- | |||
| [[Pluto]] | |||
| {{val|871|(5)}}<ref name="Buie06" /> | |||
|- | |||
| [[Eris (dwarf planet)|Eris]] | |||
| {{val|1108|(13)}}<ref name="Brown Schaller 2007" /> | |||
|} | |||
In [[celestial mechanics]], the '''standard gravitational parameter''' ''μ'' of a [[celestial body]] is the product of the [[gravitational constant]] ''G'' and the mass ''M'' of the body. | |||
:<math>\mu=GM \ </math> | |||
For several objects in the solar system, the value of ''μ'' is known to greater accuracy than ''G'' or ''M.'' The [[SI]] units of the standard gravitational parameter are [[Kilometre|km]]<sup>3</sup>[[second|s]]<sup>−2</sup>. | |||
== Small body orbiting a central body == | |||
{{Properties_of_mass}} | |||
Under standard assumptions in astrodynamics we have: | |||
: <math>m \ll M \ </math> | |||
where ''m'' is the mass of the [[orbiting body]], ''M'' is the mass of the [[central body]]. | |||
For all [[circular orbit]]s around a given central body: | |||
: <math>\mu = rv^2 = r^3\omega^2 = 4\pi^2r^3/T^2 \ </math> | |||
where ''r'' is the orbit [[radius]], ''v'' is the [[orbital speed]], ''ω'' is the [[angular speed]], and ''T'' is the [[orbital period]]. | |||
The last equation has a very simple generalization to [[elliptic orbit]]s: | |||
: <math>\mu=4\pi^2a^3/T^2 \ </math> | |||
where ''a'' is the [[semi-major axis]]. (See [[Kepler's laws of planetary motion#Kepler's third law|Kepler's third law]]). | |||
For all [[parabolic trajectory|parabolic trajectories]] ''rv''<sup>2</sup> is constant and equal to 2''μ''. For elliptic and hyperbolic orbits ''μ'' = 2''a''|''ε''|, where ''ε'' is the [[specific orbital energy]]. | |||
== Two bodies orbiting each other == <!-- This section is linked from [[Alpha Centauri]] --> | |||
In the more general case where the bodies need not be a large one and a small one (the [[two-body problem]]), we define: | |||
* the vector '''r''' is the position of one body relative to the other | |||
* ''r'', ''v'', and in the case of an [[elliptic orbit]], the [[semi-major axis]] ''a'', are defined accordingly (hence ''r'' is the distance) | |||
* ''μ'' = ''Gm''<sub>1</sub> + ''Gm''<sub>2</sub> = ''μ''<sub>1</sub> + ''μ''<sub>2</sub>, where ''m''<sub>1</sub> and ''m''<sub>2</sub> are the masses of the two bodies. | |||
Then: | |||
* for [[circular orbit]]s, ''rv''<sup>2</sup> = ''r''<sup>3</sup>''ω''<sup>2</sup> = 4π<sup>2</sup>''r''<sup>3</sup>/''T''<sup>2</sup> = ''μ'' | |||
* for [[elliptic orbit]]s, 4π<sup>2</sup>''a''<sup>3</sup>/''T''<sup>2</sup> = ''μ'' (with ''a'' expressed in AU; ''T'' in seconds and ''M'' the total mass relative to that of the Sun, we get ''a''<sup>3</sup>/''T''<sup>2</sup> = ''M'') | |||
* for [[parabolic trajectory|parabolic trajectories]], ''rv''<sup>2</sup> is constant and equal to 2''μ'' | |||
* for elliptic and hyperbolic orbits, ''μ'' is twice the semi-major axis times the absolute value of the [[specific orbital energy]], where the latter is defined as the total energy of the system divided by the [[reduced mass]]. | |||
== Terminology and accuracy == | |||
Note that the [[reduced mass]] is also denoted by <math>\mu.\!\,</math>. | |||
The value for the [[Earth]] is called the '''geocentric gravitational constant''' and equals {{val|398600.4418|0.0008|u=km<sup>3</sup>s<sup>−2</sup>}}. Thus the uncertainty is 1 to {{val|500000000}}, much smaller than the uncertainties in ''G'' and ''M'' separately (1 to {{val|7000}} each). | |||
The value for the [[Sun]] is called the '''heliocentric gravitational constant''' or | |||
''geopotential of the sun'' and equals {{val|1.32712440018|e=20|u=m<sup>3</sup>s<sup>−2</sup>}}. | |||
== References == | |||
{{reflist | |||
| refs = | |||
<ref name="Astrodynamic Constants"> | |||
{{cite web | |||
| title = Astrodynamic Constants | |||
| date = 27 February 2009 | |||
| publisher = [[NASA]]/[[Jet Propulsion Laboratory|JPL]] | |||
| url = http://ssd.jpl.nasa.gov/?constants | |||
| accessdate = 27 July 2009 | |||
}} | |||
</ref> | |||
<ref name="Pitjeva2005"> | |||
{{cite journal | |||
| doi = 10.1007/s11208-005-0033-2 | |||
| author = E.V. Pitjeva | |||
| year = 2005 | |||
| title = High-Precision Ephemerides of Planets — EPM and Determination of Some Astronomical Constants | |||
| url = http://iau-comm4.jpl.nasa.gov/EPM2004.pdf | |||
| journal = [[Solar System Research]] | |||
| volume = 39 | |||
| issue=3 | |||
| pages=176 | |||
| bibcode = 2005SoSyR..39..176P | |||
}} | |||
</ref> | |||
<ref name="Britt2002"> | |||
{{cite book | |||
| author = D. T. Britt, D. Yeomans, K. Housen, G. Consolmagno | |||
| year = 2002 | |||
| chapter = Asteroid density, porosity, and structure | |||
| title = [http://www.lpi.usra.edu/books/AsteroidsIII/download.html Asteroids III] | |||
| editor = W. Bottke, A. Cellino, P. Paolicchi, R.P. Binzel | |||
| page = 488 | |||
| publisher = [[University of Arizona Press]] | |||
| url = http://www.lpi.usra.edu/books/AsteroidsIII/pdf/3022.pdf | |||
}} | |||
</ref> | |||
<ref name="Jacobson1992"> | |||
{{cite journal | |||
| doi = 10.1086/116211 | |||
| author = R.A. Jacobson, J.K. Campbell, A.H. Taylor, S.P. Synnott | |||
| year = 1992 | |||
| title = The masses of Uranus and its major satellites from Voyager tracking data and Earth-based Uranian satellite data | |||
| journal = [[Astronomical Journal]] | |||
| volume = 103 | |||
| issue = 6 | |||
| pages = 2068–2078 | |||
| bibcode = 1992AJ....103.2068J | |||
}} | |||
</ref> | |||
<ref name="Buie06"> | |||
{{cite journal | |||
| doi = 10.1086/504422 | |||
| author = M.W. Buie, W.M. Grundy, E.F. Young, L.A. Young, S.A. Stern | |||
| year = 2006 | |||
| title = Orbits and photometry of Pluto's satellites: Charon, S/2005 P1, and S/2005 P2 | |||
| journal = [[Astronomical Journal]] | |||
| volume = 132 | |||
| pages = 290 | |||
| bibcode = 2006AJ....132..290B | |||
| arxiv = astro-ph/0512491 | |||
}} | |||
</ref> | |||
<ref name="Brown Schaller 2007"> | |||
{{cite journal | |||
| doi = 10.1126/science.1139415 | |||
| author = M.E. Brown, E.L. Schaller | |||
| year = 2007 | |||
| title = The Mass of Dwarf Planet Eris | |||
| journal = [[Science (journal)|Science]] | |||
| volume = 316 | |||
| issue = 5831 | |||
| pages = 1586 | |||
| bibcode = :2007Sci...316.1585B | |||
}} | |||
</ref> | |||
<!-- | |||
<ref name="Lunar Constants and Models Document"> | |||
{{cite web | |||
| title = Lunar Constants and Models Document | |||
| date = 23 September 2005 | |||
| publisher = [[NASA]]/[[Jet Propulsion Laboratory|JPL]] | |||
| url = http://www.hq.nasa.gov/alsj/lunar_cmd_2005_jpl_d32296.pdf | |||
| accessdate = 1 April 2013 | |||
}} | |||
</ref>--> | |||
}} | |||
== See also == | |||
* [[Astronomical system of units]] | |||
* [[Planetary mass]] | |||
{{orbits}} | |||
[[Category:Orbits]] |
Revision as of 01:20, 14 January 2014
In celestial mechanics, the standard gravitational parameter μ of a celestial body is the product of the gravitational constant G and the mass M of the body.
For several objects in the solar system, the value of μ is known to greater accuracy than G or M. The SI units of the standard gravitational parameter are km3s−2.
Small body orbiting a central body
Template:Properties of mass Under standard assumptions in astrodynamics we have:
where m is the mass of the orbiting body, M is the mass of the central body.
For all circular orbits around a given central body:
where r is the orbit radius, v is the orbital speed, ω is the angular speed, and T is the orbital period.
The last equation has a very simple generalization to elliptic orbits:
where a is the semi-major axis. (See Kepler's third law).
For all parabolic trajectories rv2 is constant and equal to 2μ. For elliptic and hyperbolic orbits μ = 2a|ε|, where ε is the specific orbital energy.
Two bodies orbiting each other
In the more general case where the bodies need not be a large one and a small one (the two-body problem), we define:
- the vector r is the position of one body relative to the other
- r, v, and in the case of an elliptic orbit, the semi-major axis a, are defined accordingly (hence r is the distance)
- μ = Gm1 + Gm2 = μ1 + μ2, where m1 and m2 are the masses of the two bodies.
Then:
- for circular orbits, rv2 = r3ω2 = 4π2r3/T2 = μ
- for elliptic orbits, 4π2a3/T2 = μ (with a expressed in AU; T in seconds and M the total mass relative to that of the Sun, we get a3/T2 = M)
- for parabolic trajectories, rv2 is constant and equal to 2μ
- for elliptic and hyperbolic orbits, μ is twice the semi-major axis times the absolute value of the specific orbital energy, where the latter is defined as the total energy of the system divided by the reduced mass.
Terminology and accuracy
Note that the reduced mass is also denoted by .
The value for the Earth is called the geocentric gravitational constant and equals Template:Val. Thus the uncertainty is 1 to Template:Val, much smaller than the uncertainties in G and M separately (1 to Template:Val each).
The value for the Sun is called the heliocentric gravitational constant or geopotential of the sun and equals Template:Val.
References
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See also
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