 |  |
Astron. Astrophys. 329, 840-844 (1998)
4. Results and conclusions
We have developed a method to estimate the combined effect of
extinction and inclination of the galactic disk on the luminosity
function. The magnitude of the effect depends on the amount of opaque
matter present in the disk. We have assumed exponential laws for the
optical depth and the emission coefficent : . We
have seen in Sect. (3.1) that an inhomogeneous model with
parameters is equivalent to an homogeneous
slab with mean opacity given by the Eq.
.
In Fig. 1 we show the corrected LF when the observed LF has
been modeled by a gaussian with a mean of mag.
We have considered two values for the mean optical depth
and . One sees a growth
in the number of brilliant galaxies. This increment is compensated by
a diminution in the faint end, under the inflexion points of the
gaussian In Fig. 2 we show the corrected LF when the observed LF
is a Schechter function. We have considered three different values of
the mean optical depth, ,
, , and, the case
has also been included in order to compare
with the previous paper (Leroy & Portilla 1996).
![[FIGURE]](img121.gif) |
Fig. 1. One shows the corrected LF when the observed LF is a gaussian with a mean of mag . We assume the inclination i uniformly distributed. The dotted line corresponds to a mean opacity , and the dashed line to .
|
![[FIGURE]](img126.gif) |
Fig. 2. One shows the corrected LF when the observed LF is a Schechter function, assuming the inclination i of the galactic plane uniformly distributed, for three different values of the mean optical depth. The dash-dot line corresponds to , the dashed line to , and the dash-three dots line to . The solid line represents the Schechter function, and the dotted line represents the correction for inclination effect in the case of infinite opacity.
|
The extinction effect is manifested as a shift of the Schechter
function towards the left of the figure. For small opacities
( ) we observe the extinction shift to the left,
plus a slight growth in the number of faint galaxies (the opacity is
too small to change the number of bright galaxies for the effect of
inclination). This changes for . One recognizes
now the inclination effect as an increase in the number of bright
galaxies and a decrease in the number of faint ones. In the same
figure we show the inclination effect in the case of infinite optical
depth. We have obtained similar results (Fig. 3) assuming that
the variable is uniformly distributed. In a
recent paper (Leroy & Portilla 1996) we used the results for
infinite optical depth to study the influence of the opacity on the
faint galaxy number counts. The results obtained in this work indicate
that the combined effect of a finite optical depth plus the extinction
correction is similar to the inclination effect in the case of
infinite opacity. We are using the results of this paper to estimate
the mean luminosity density and the mass luminosity ratio. The
selection function may also be influenced by these effects.
![[FIGURE]](img131.gif) |
Fig. 3. One shows the corrected luminosity function when the observed LF is a Schechter function, assuming uniformly distributed, for two different values of the mean optical depth. The dash-dot line corresponds to ,and the dashed line to . The solid line and the dotted line represent the same as in Fig. 2.
|
© European Southern Observatory (ESO) 1998
Online publication: December 16, 1997
helpdesk.link@springer.de  |