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Models of surface brightness profiles
No physical law exists which describes the surface brightness profile of a galaxy. Initially Patterson patterson1940 and later De Vaucouleurs vaucouleurs1959 showed that surface brightness profiles could be described by an exponential function. Even later Freeman freeman1970 surveyed the literature to show empirically this exponential behaviour on face-on disk galaxies and coupled the exponential function with a dynamical background, establishing its form as we know it up to today as
  | 
(2) | 
 
where 
 is the radial position from the center of the disk and 
 the radial scalelength, and 
 the central surface brightness.
Van der Kruit vdkruit1979 showed that the surface brightness in 
 is independent of 
 and that the vertical profile can be described by an analogue exponential function using the vertical scaleheight as a parameter. In an attempt to fit the 
 distribution of light at each 
 by that of a locally isothermal sheet, Van der Kruit & Searle vdkruit1981a found that a sech
 (
) function was a more appropriate description for the vertical surface brightness profile. Some years later Van der Kruit vdkruit1988 proposed to use a sech function as an intermediate solution to fit vertical profile as he showed that the exponential and the sech
 function all belonged to the same family of density laws
  | 
(3) | 
 
where 
 is the observed vertical density profile and 
 the scaleheight, while 
 is the distance from the plane. The isothermal model is the extreme for 
 = 1 and the exponential is the other extreme for 
. With this family of density laws, there are several ways to determine structural parameters.
Figure:
Radial profiles of NGC 5290 J at the midplane and at vertical positions above and below the plane. The magenta line shows 
.
 
 | 
Figure:
Vertical profiles of NGC 5290 J at the center and at two radial positions on the left and right side from the center. The magenta line shows 
.
 
 | 
 
 
 
 
  
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O.A. van den  Berg
2006-09-05