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Astron. Astrophys. 345, 925-935 (1999)
5. Conclusion
Within the uncertainties encountered in the observations as
discussed, Figs. 1, 2 & 4 and Tables 1-3 show acceptable
comparisons between the predicted and observed integrated
H2O spectra and FIR continua. The error bars for observed
SWS line fluxes are nevertheless high by a factor 2-3; and it is
interesting to perform new observations in this wavelength region.
Some CO and CII lines are also found in the H2O spectra but
their investigation is outside the scope of this paper. Observations I
show a spectrum about 30-40% less
intense compared to Observations II's where new or stronger lines
appear and some components of a blend become clearly visible. This
light variation due to stellar pulsations of the Mira variable between
300 days corresponds to a phase
variation from 0.5, at minimum luminosity, to 0.2 where the luminosity
was falling down to its mean value. A best fit to the overall spectra
were obtained with the dilution factor for the FIR field scaled by a
factor 0.61 and 1, respectively. This
FIR field is mainly dominated by dust. Photodissociation of
H2O by the interstellar UV field does not affect
significantly the FIR H2O line fluxes, since the effect
operates in the outer region (
cm) where H2O excitation
temperatures become weak. The derived H2O abundance and
density, the FIR continuum, and the kinetic temperature vary as
functions of radius across the circumstellar envelope of R Cas.
The derived mass-loss rate is
3.4![[FORMULA]](img5.gif)
. The deduced total (ortho and
para) H2O abundance is
1.1![[FORMULA]](img5.gif)
and the kinetic temperature is
1300 K at the inner radius of the
envelope, and they decrease with distance from the star. Compared to
W Hya, another O-rich AGB star, the initial H2O
abundance of R Cas is about one order of magnitude lower while
the mass-loss rate is nearly the same; the values found for W Hya
(1.2![[FORMULA]](img5.gif)
and 6![[FORMULA]](img5.gif)
; see Barlow et al. 1996) were
determined, however, by using a different model. Similar mass-loss
rates (
) have been derived for a number of
LPV Miras using CO radio observations (e.g. Knapp et al. 1982, Loup et
al. 1993, Kahane & Jura 1994, Gonzalez-Alfonso et al. 1998), and
optical KI /NaI scattering (e.g. Guilain
& Mauron 1996).
© European Southern Observatory (ESO) 1999
Online publication: April 28, 1999
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