![]() | Annu. Rev. Astron. Astrophys. 1996. 34:
155-206 Copyright © 1996 by Annual Reviews. All rights reserved |
Mean equipartition strengths of the total field
<B3+s>1 /
(3+
s)
(averaged over the
volume of the visible radio disk) range from
4 µG in M33
(Buczilowski & Beck
1991)
to
12 µG in
NGC 6946 and NGC 1566
Ehle & Beak,
Ehle et al 1996);
they are proportional to surface brightness in the far-infrared range
(Hummel et al 1988b)
and to average gas density (S Niklas et al, in preparation)
Hummel's (1986)
sample of 88 Sbc galaxies has a mean minimum-energy field of
8 µG, using
K = 100. Using the same value of K for the sample of 146
late-type galaxies by
Fitt & Alexander
(1993), one obtains a mean total minimum-energy field strength of 10
± 4 µG.
Extremal values found in normal galaxies can be up to
20 µG in spiral arms, as in NGC 6946
(Beck 1991) and
NGC 1566
(Ehle et al 1996).
In the mildly active galaxy M82,
Klein et al (1988)
found a field strength
50 µG.
The regular field strengths
as obtained from
the intensity of polarized emission are typically a few µG.
Such values are roughly consistent with regular field strengths
|| as
derived from Faraday rotation data, if we assume
typical electron densities of a few 10-2 cm-3 (see
e.g.
Buczilowski & Beck
1991). Because polarized
intensity and rotation measure depend differently
on the filling factor of the field, the fact that
|| implies
that the filling factor is not very small.
The ratio of regular to turbulent field strengths is typically
0.5 if observed with a
spatial resolution of a few kpc
(Buczilowski & Beck
1991).
In NGC 2276 the regular field strength reaches 10 µG (Hummel & Beck 1995), probably due to its interaction with the ambient intracluster gas. The total field is also unusually strong in that galaxy. Galaxies in clusters generally contain stronger fields (Gavazzi et al 1991, Niklas et al 1995).