Cyclic changes in dust-to-gas ratio

Authors
Citation
H. Hirashita, Cyclic changes in dust-to-gas ratio, ASTROPHYS J, 531(2), 2000, pp. 693-700
Citations number
38
Categorie Soggetti
Space Sciences
Journal title
ASTROPHYSICAL JOURNAL
ISSN journal
0004637X → ACNP
Volume
531
Issue
2
Year of publication
2000
Part
1
Pages
693 - 700
Database
ISI
SICI code
0004-637X(20000310)531:2<693:CCIDR>2.0.ZU;2-Y
Abstract
We discuss the time variation of the dust-to-gas mass ratio in spiral galax ies, using the multiphase model of interstellar medium. The typical timesca le of the phase change of an interstellar gas is similar to 10(7-8) yr in s piral galaxies. Since the phase transition changes the filling factor of th e cold gas where the dust growth occurs, the dust growth rate varies on tha t timescale. In order to examine the response of the dust-to-gas ratio to t he phase transition, we construct a model of the time evolution of the dust -to-gas ratio. We adopt the three-phase model for the interstellar gas and the Ikeuchi-Tomita model for the mass exchange between the phases. Accordin g to the model, three types of solutions are possible: (1) all the gas is t ransformed to a hot gas; (2) a stable stationary state of three phases is r ealized; and (3) the filling factor of each phase cyclically changes. For t he three types of solutions, the dust-to-gas ratio behaves as follows: for solution 1, almost all the dust is destroyed (the dust-to-gas ratio becomes similar to 0); for solution 2, the dust-to-gas ratio converges to a statio nary state; and for solution 3, the dust-to-gas ratio varies cyclically In response to the phase transition. In the case of solution 3, the amplitude of the variation of the dust-to-gas ratio is large (nearly an order of magn itude) if the dust growth timescale is shorter than the phase transition ti mescale. This condition is easily satisfied in spiral galaxies. However, it is difficult for dwarf galaxies to realize the condition, because their sm all metallicity makes the dust growth timescale long.