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The radiation from ordinary galaxies is dominated by thermal
radiation from stars and dust. Active galaxies are dominated
by non-thermal processes like synchrotron radiation and thyermal
processes with exceedingly high temperatures (i.e. large energies).
Activity is often indicated by the presence of emission lines
in the spectrum of the object.
The temperatures involved vary from about 100°K for the
dust in the interstellar medium to several thousand degrees for
stellar photospheres. Stars generally fall in the range between
3000° and 30000° K. Stars emit most of their energy
near the visual wavelength region. The hottest stars actually
have their peak emission in the UV while the coolest stars have
their peak emission in the near-IR to mid-IR.
The Wien displacement rule describes the relationship between
the temperature of a thermal source and the wavelength of the
peak emission.
lmax = 2898 / T (in mm)
Here T is the temperature in °K.
|
T (°K) |
lmax (mm) |
|
100 |
29.0 |
|
3000 |
0.97 |
|
6000 |
0.48 |
|
30000 |
0.097 |
At wavelengths longer than the peak the radiation emitted decreases
slowly with increasing wavelength. (At wavelengths shorter than
the peak there is a rapid decrease.) At radio wavelengths (or
frequencies) we are observing on the long wavelength tail of
the energy distribution for ordinary stellar and galactic sources.
Thus, in the radio region, ordinary astronomical sources which
are thermal emitters are brighter at higher frequencies (shorter
wavelengths).
Synchrotron radiation is produced when energetic electrons
move through a region of space containing a magnetic field. The
motions of the electrons are deflected by the magnetic field
and the electrons spiral around the magnetic field lines. Since
circularily moving electrons are being accelerated, these electrons
emit radiation. The spectral distribution of this radiation may
be described by the following relation.
F(n) = F0 n-a = F0 / na
Here a is termed the spectral index of the radiation. This
index may be related to the energy distribution of the electrons
producing the radiation, and to the strength and uniformity of
the magnetic field. Radio galaxies and quasars have similar radio
properties and have spectral indices between 0.7 and 1.2. Compact
radio sources have a flatter spectrum and tend to have a spectral
index near a = 0.4. Note that in this system thermal sources
have negative spectral indices.
Synchrotron sources decrease in brightness at higher frequencies,
while thermal sources increase in brightness.
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