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Astron. Astrophys. 351, 495-505 (1999)
4. A lower limit to grain temperature
We found very cold dust in all inactive spirals of our
sample. One may wonder whether still colder dust might exist that has
escaped detection. To partially answer this question, we compute under
reasonable assumptions a lower limit,
, to the temperature of a grain in a
disk galaxy. Very cold dust must be well protected from direct
starlight, mag, and can only be
found inside clouds. Such clouds are nevertheless transparent to FIR
emission of the galaxy itself, at least for wavelengths above
25 µm. In this range, the optical depth is according to
most dust models over 50 times smaller than in the visual (e.g.
Draine 1985, Zubko et al. 1996). To minimize the FIR
heating, which is rather inefficient anyway because of small
absorption cross sections, we adopt the source of FIR radiation to
reside in the galactic nucleus of say the central 500 pc. Heating by
radiation at shorter wavelengths and/or spatially spread-out energy
sources, like stars in the disk, would increase the estimate for
.
As is appropriate for most inactive spirals, we assume a
spectral shape for the FIR radiation
with K. Fig. 16 gives a flavor of
the minimum dust temperature as a function of galactocentric radius.
If the total FIR luminosity is
, as
in the Milky Way, the dust in the disk within a radius of 15 kpc,
which is a typical optical radius of a galaxy, cannot become colder
than K. In addition, one may use
this figure to get an impression on where to find the bulk of the very
cold component of the ISM. Fig. 16 also shows the variation of
with
.
![[FIGURE]](img127.gif) |
Fig. 16. Minimum dust temperature as a function of galactocentric radius for , and , respectively.
|
Fig. 16 is almost independent of the size or composition of grains.
Only a -variation of the absorption
efficiency at long wavelengths is required because for the deeply
buried dust both absorption and emission occur in the FIR and it is
just the slope, not the absolute value of the absorption efficiency
that determines . The grain model,
however, has an influence on the derived dust mass. If the very cold
dust is fluffy and icy, or has an elongated form, its millimeter
absorption coefficient is enhanced relative to that of the standard
dust by some factor (Krügel & Siebenmorgen 1994,
Ossenkopf & Henning 1994) and the mass will be overestimated
by exactly this amount.
© European Southern Observatory (ESO) 1999
Online publication: November 3, 1999
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