2.2. Disc Galaxies
Spiral galaxies possess a flat disc component which follows closely an exponential light distribution,
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(2.12) |
(Freeman, 1970).
The central surface brightness appears to be
constant, close to I0 = 145
L
pc-2 (Freeman's law). The spirals also
possess a spheroidal component (bulge) which obeys the
r1/4 law
(Eq. 2.1). The ratio of the light in the disc (LD) to
the light in the
bulge (LB) is one of the parameters used to determine the
classification stage of a spiral, the others being the openness of the
spiral pattern and the degree of resolution of the arms into bright
stars. These quantities increase from early to late type spirals,
i.e. along the stage designations a-d.
The lenticular galaxies (designated SO) are similar to spirals in
that they have both a spheroidal component and an exponential
disc. They differ in that SO's generally have no spiral arms and
contain little gas.
The disc galaxies are divided into families according to whether or
not they possess a bar. Barred galaxies are not uncommon. Disc
galaxies are fairly evenly distributed between the unbarred (SA, SAO),
intermediate (SAB, SABO) and barred (SB, SBO) families.
From a detailed photometric study of 12 lenticular galaxies,
Burstein (1979)
finds that on average SO's have larger bulge to disc
ratios than do spirals. Also, the central surface brightness of the
disc components are fairly evenly distributed between
µ0
- 20.1 and
-22.1 B mag/square-arcsec and do not peak around the value
µ0 = - 21.65
Bmag/squ. arcsec expected from Freeman's law. It has been suggested
that Freeman's law is an artifact of the selection criteria used to
identify galaxies as suitable candidates for detailed photometric
study. For example, if a galaxy were of low surface brightness, it
would be difficult to detect above the sky background, whilst if a
galaxy were of high surface brightness it might be difficult to
distinguish from a star.
Disney (1976)
has used this argument to show
that galaxies on the Palomar sky survey plates would have a maximum
apparent diameter if
µ0 = - 21.6, stingly close to the value obtained
by Freeman. This effect has been considered by
Bosma and Freeman (1981)
who have searched the much deeper UK sky survey plates in an
attempt to find giant low surface brightness spirals. Few such objects
have been found and their results support Freeman's law. Another
criticism levelled at Freeman's result concerns errors introduced into
the disc parameters I0 and
(Eq. 2.12) due to the
presence of the bulge component
(Kormendy, 1977b).
Boroson (1981)
has made a
photometric study of spiral galaxies with particular emphasis on this
problem. He finds that the distribution of central surface
brightnesses peaks at the value given by Freeman's law, though the
scatter is larger than that found by Freeman.
Freeman did identify a few galaxies with high surface brightness
µ0
18
Bmag/squ. arcsec. These galaxies all have luminosity profiles
designated by Freeman as Type II. For most spirals (Type I profiles),
the extrapolation of the exponential component into the centre of the
galaxy is always fainter than the measured brightness profile. Type II
profiles dip below the extrapolation of the exponential towards the
centre.
Talbot, Jensen and Dufour
(1979)
have used multicolour photometry in a
study of NGC 5236 (M83). Freeman's model Type II galaxy. They
find that the Type II behaviour is probably due to the presence of young
blue stars and that the underlying old stellar population has a
typical Type I profile.