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Standard gravitational parameter

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Body μ (km3s-2)
Sun 132,712,440,018
Mercury 22,032
Venus 324,859
Earth 398,600 .4418 ±0.0008
Moon 4902 .7779
Mars 42,828
Ceres 63 .1 ±0.3[1][2]
Jupiter 126,686,534
Saturn 37,931,187
Uranus 5,793,939 ± 13[3]
Neptune 6,836,529
Pluto 871 ±5[4]
Eris 1,108 ±13[5]

In astrodynamics, the standard gravitational parameter \mu \ of a celestial body is the product of the gravitational constant G and the mass M:

\mu=GM \

The units of the standard gravitational parameter are km3s-2


Contents

[edit] Small body orbiting a central body

The above diagram illustrates five interrelated properties of mass together with the proportionality constants that relate these properties. Every sample of mass is believed to exhibit all five properties, however, due to extremely large proportionality constants, it is generally impossible to verify more than two or three properties for a specific sample of mass.
  • The Schwarzschild radius (rs) represents the ability of mass to cause curvature in space and time.
  • The standard gravitational parameter (μ) represents the ability of a massive body to exert Newtonian gravitational forces on other bodies.
  • Inertial mass (m) represents the Newtonian response of mass to forces.
  • Rest energy (E0) represents the ability of mass to be converted into other forms of energy.
  • The Compton wavelength (λ) represents the quantum response of mass to local geometry.

Under standard assumptions in astrodynamics we have:

m << M \

where:

and the relevant standard gravitational parameter is that of the larger body.


For all circular orbits around a given central body:

\mu = rv^2 = r^3\omega^2 = 4\pi^2r^3/T^2 \

where:


The last equality has a very simple generalization to elliptic orbits:

\mu=4\pi^2a^3/T^2 \

where:

See Kepler's third law.


For all parabolic trajectories r v^2 \ is constant and equal to 2 \mu \ ;.

For elliptic and hyperbolic orbits  \mu \ is twice the semi-major axis times the absolute value of the specific orbital energy.

[edit] Two bodies orbiting each other

In the more general case where the bodies need not be a large one and a small one, we define:

  • the vector  \mathbf{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)
  • \mu={G}(m_1 + m_2) \ (the sum of the two  \mu \ values)

where:

  • m_1 \ and m_2 \ are the masses of the two bodies.

Then:

[edit] Terminology and accuracy

The value for the Earth is called geocentric gravitational constant and equal to 398 600.441 8 ± 0.000 8 km3s-2. Thus the uncertainty is 1 to 500 000 000, much smaller than the uncertainties in G and M separately (1 to 7000 each).

The value for the Sun is called heliocentric gravitational constant and equals 1.32712440018 × 1020 m3s-2.


[edit] References

  1. ^ Pitjeva, E. V. (2005). "High-Precision Ephemerides of Planets — EPM and Determination of Some Astronomical Constants" (PDF). Solar System Research 39 (3): 176. doi:10.1007/s11208-005-0033-2. http://iau-comm4.jpl.nasa.gov/EPM2004.pdf. 
  2. ^ D. T. Britt et al Asteroid density, porosity, and structure, pp. 488 in Asteroids III, University of Arizona Press (2002).
  3. ^ Jacobson, R.A.; Campbell, J.K.; Taylor, A.H.; Synnott, S.P. (1992). "The masses of Uranus and its major satellites from Voyager tracking data and Earth-based Uranian satellite data". The Astronomical Journal 103 (6): 2068–2078. doi:10.1086/116211. http://adsabs.harvard.edu/abs/1992AJ....103.2068J. 
  4. ^ M. W. Buie, W. M. Grundy, E. F. Young, L. A. Young, S. A. Stern (2006). "Orbits and photometry of Pluto's satellites: Charon, S/2005 P1, and S/2005 P2". Astronomical Journal 132: 290. doi:10.1086/504422. arΧiv:astro-ph/0512491. http://adsabs.harvard.edu/cgi-bin/nph-bib_query?bibcode=2006AJ....132..290B&db_key=AST&data_type=HTML&format=&high=444b66a47d27727. 
  5. ^ M.E. Brown and E.L. Schaller (2007). "The Mass of Dwarf Planet Eris". Science 316 (5831): 1585. doi:10.1126/science.1139415. PMID 17569855. http://www.sciencemag.org/cgi/content/full/316/5831/1585. 
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