Virial mass

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In astrophysics, the virial mass is the mass of a gravitationally bound astrophysical system, assuming the virial theorem applies. In the context of galaxy formation and dark matter halos, the virial mass is defined as the mass enclosed within the virial radius of a gravitationally bound system, a radius within which the system obeys the virial theorem. The virial radius is determined using a "top-hat" model. A spherical "top hat" density perturbation destined to become a galaxy begins to expand, but the expansion is halted and reversed due to the mass collapsing under gravity until the sphere reaches virial equilibrium–it is said to be virialized. Within this radius, the sphere obeys the virial theorem which says that the average kinetic energy is equal to minus one half times the average potential energy, , and this radius defines the virial radius.

Virial radius[edit]

The virial radius of a gravitationally bound astrophysical system is the radius within which the virial theorem applies. It is defined as the radius at which the density is equal to the critical density of the Universe at the redshift of the system, multiplied by an overdensity constant :

where is the halo's mean density within that radius, is a parameter, is the critical density of the Universe, is the Hubble parameter, and is the virial radius.[1][2] The time dependence of the Hubble parameter indicates that the redshift of the system is important, as the Hubble parameter changes with time: today's Hubble parameter, referred to as the Hubble constant , is not the same as the Hubble parameter at an earlier time in the Universe's history, or in other words, at a different redshift. The overdensity is given by

where , and .[3][4] Since it depends on the density parameter , its value depends on the cosmological model used. In an Einstein–de Sitter model it equals . This definition is not universal, however, as the exact value of depends on the cosmology. In an Einstein–de Sitter model, it is assumed that the density parameter is due to matter only, where . Compare this to the currently accepted cosmological model for the Universe, ΛCDM model, where and ; in this case, . Nevertheless, it is typically assumed that for the purpose of using a common definition, and this is denoted as for the virial radius and for the virial mass. Using this convention, the mean density is given by

Other conventions for the overdensity constant include , or , depending on the type of analysis being done, in which case the virial radius and virial mass is signified by the relevant subscript.[2]

Defining the virial mass[edit]

Given the virial radius and the overdensity convention, the virial mass can be found through the relation

If the convention that is used, then this becomes[1]
where is the Hubble parameter as described above, and G is the gravitational constant. This defines the virial mass of an astrophysical system.

Applications to dark matter halos[edit]

Given and , properties of dark matter halos can be defined, including circular velocity, the density profile, and total mass. and are directly related to the Navarro–Frenk–White (NFW) profile, a density profile that describes dark matter halos modeled with the cold dark matter paradigm. The NFW profile is given by

where is the critical density, and the overdensity (not to be confused with ) and the scale radius are unique to each halo, and the concentration parameter is given by .[5] In place of , is often used, where is a parameter unique to each halo. The total mass of the dark matter halo can then be computed by integrating over the volume of the density out to the virial radius :

From the definition of the circular velocity, we can find the circular velocity at the virial radius :

Then the circular velocity for the dark matter halo is given by
where .[5]

Although the NFW profile is commonly used, other profiles like the Einasto profile and profiles that take into account the adiabatic contraction of the dark matter due to the baryonic content are also used to characterize dark matter halos.

To compute the total mass of the system, including stars, gas, and dark matter, the Jeans equations need to be used with density profiles for each component.

See also[edit]


  1. ^ a b Sparke, Linda S.; Gallagher, John S. (2007). Galaxies and the Universe. United States of America: Cambridge University Press. pp. 329, 331, 362. ISBN 978-0-521-67186-6.
  2. ^ a b White, M (3 February 2001). "The mass of a halo". Astronomy and Astrophysics. 367 (1): 27–32. arXiv:astro-ph/0011495. Bibcode:2001A&A...367...27W. doi:10.1051/0004-6361:20000357.
  3. ^ Bryan, Greg L.; Norman, Michael L. (10 Oct 1997). "Statistical Properties of X-ray Clusters: Analytic and Numerical Comparisons". The Astrophysical Journal. 495 (80): 80. arXiv:astro-ph/9710107. Bibcode:1998ApJ...495...80B. doi:10.1086/305262.
  4. ^ Mo, Houjun; van den Bosch, Frank; White, Simon (2011). Galaxy Formation and Evolution. United States of America: Cambridge University Press. p. 236. ISBN 978-0-521-85793-2.
  5. ^ a b Navarro, Julio F.; Frenk, Carlos S.; White, Simon D. M. (7 Aug 1995). "The Structure of Cold Dark Matter Halos". The Astrophysical Journal. 462: 563–575. arXiv:astro-ph/9508025. Bibcode:1996ApJ...462..563N. doi:10.1086/177173.