Astron. Astrophys. 336, 823-828 (1998)
6. Dust mass
The mass of dust associated with the near-infrared emission can be
only roughly estimated, because it depends on the (unknown) grain
sizes and composition. Assuming graphite grains and following
Barvainis (1987), the infrared spectral luminosity of an individual
graphite grain is given by:
![[EQUATION]](img25.gif)
where a is the grain radius, is the
absorption efficiency of the grains, and is the
Planck function for a grain temperature .
Following Barvainis (1987), we take a=0.05 µm and
=0.058. With =900 K, we
find .
In NGC 7469 the K band flux is
=2.2 10-25 ergs s-
1 cm-2 Hz-1, at a distance
D=66 Mpc. We derive the number of hot
( =900 K) grains: n=7.58 1046.
Taking a grain density
=2.26 g cm-3, we get:
M(hot dust)
0.05 . This result is comparable to the
0.02 mass of hot dust found in another
Seyfert 1 nucleus, Fairall 9 (Clavel et al., 1989), but substantially
larger than in other AGN: 2.5 10 in NGC 3783
(Glass, 1992), 7 10 in NGC 1566 (Baribaud et
al., 1992) and 5 10 in NGC 4593
(Santos-Lléo et al., 1995).
© European Southern Observatory (ESO) 1998
Online publication: July 27, 1998
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