1988
DOI: 10.1086/166378
|View full text |Cite
|
Sign up to set email alerts
|

Dynamical modeling of long-period variable star atmospheres

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

21
541
1

Year Published

1993
1993
2015
2015

Publication Types

Select...
5
3

Relationship

0
8

Authors

Journals

citations
Cited by 497 publications
(565 citation statements)
references
References 0 publications
21
541
1
Order By: Relevance
“…This model represented the maser clumps as LVG blocks with physical conditions drawn from a pulsating atmosphere model of a Mira variable (Bowen 1988). The pulsating atmosphere provides radial shock-waves, attenuating with increasing radius.…”
Section: Water Maser Theory and Modellingmentioning
confidence: 99%
“…This model represented the maser clumps as LVG blocks with physical conditions drawn from a pulsating atmosphere model of a Mira variable (Bowen 1988). The pulsating atmosphere provides radial shock-waves, attenuating with increasing radius.…”
Section: Water Maser Theory and Modellingmentioning
confidence: 99%
“…The computational improvements can be inferred by comparing these results with the radial structures depicted e.g. in Bowen (1988, Fig. 6-8, calculated for similar initial conditions using a much simpler Lagrangian numerical scheme).…”
Section: Resultsmentioning
confidence: 96%
“…For the equation of state we assume a perfect gas law (7 = 5/3, /i = 1.3), the Rosseland mean of the gas opacity is set to the constant value of 10~4 g/cm 3 and the dust opacity is calculated by the simple formula given in Bowen (1988).…”
Section: Basic Physics and Numerical Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…Part of the line was found to originate in near-photospheric circumstellar material slightly shifted in velocity relative to the photosphere. It had earlier been suggested that if H2 is produced by three-body recombination, the recombination would be so slow in the low densities in mira atmospheres that H would remain neutral (not associated) between shocks (Bowen 1988). However, these observations disclose that, after the passage of a pulsationally driven shock through the atmosphere, the H2 lines reappear almost as quickly as do CO and TiO lines, forcing the conclusion that recombination proceeds more rapidly than expected, which in turn demands higher densities of H I or consideration of processes other than three-body recombination.…”
Section: Hmentioning
confidence: 99%