Astron. Astrophys. 364, L97-L100 (2000)
2. The PA-inclination method
The 3-dimensional orientation of the SV of a galaxy is
characterized by two angles: the polar angle
between the galactic SV and a
reference plane, and the azimuthal angle
between the projection of the
galactic SV on to this reference plane and the X-axis within this
plane. When using the Local Supercluster (LSC) as reference, then
and
can be obtained from measurable quantities as follows (Flin & Godl
owski 1986):
![[EQUATION]](img3.gif)
where i is the inclination angle, estimated with Holmberg's
(1946) formula: with
being the measured axial ratio.
L, B and P represent the supergalactic longitude,
latitude, and position angle, respectively.
Note, that for a given value of i, these expressions give
two solutions for both and
and hence 4 solutions for the angular
momentum vector of the galaxy. However, for a large sample of galaxies
it is hardly possible to determine - for each galaxy - which one is
the physical correct one. As usual we have counted each of these
possibilities independently.
Note further, that Eqs. (1) and (2) will give one single
solution for both and
when a galaxy is seen exactly face-on
( ). When seen edge-on
( ), the two solutions for both
and
differ just in sign.
More interestingly, the characteristics of the solutions for
and
are also strongly influenced by the used coordinate system. This was
already noted by Flin & Godl owski 1986 (their Sect. 6.1).
These authors suggested an analytical method to remove these selection
effects due to positions. In the case of
, both solutions converge when
approaching the supergalactic pole or for galaxies with supergalactic
PA . In the case of
both solutions just differ in sign
for . As an example, let a galaxy
cluster of small angular size be filled with galaxies whose SVs are
randomly distributed in space. The distribution of the calculated
angles and
will then depend on the position of
that cluster on the celestial sphere. Consequently, when considering a
larger region the expected distribution of
and
will be defined by the location of that region on the sky, but also by
its boundaries.
Mathematically, the expected distribution of the calculated values
of and
, when applying the expressions (1)
and (2), is determined by the assumed spatial distribution of the SVs
of the galaxies and the interval from which the variables L,
B, P, and i have been taken. The latter influence
is what we call selection effect in the following.
Due to the special form of the expressions (1) and (2) these
selection effects cannot in general be calculated analytically. In
order to minimize the selection effects due to positions and
inclination angles we have done numerical simulations.
© European Southern Observatory (ESO) 2000
Online publication: January 29, 2001
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