DUST ENVELOPES AROUND THE SECONDARY COMPONENTS OF BM ORI AND V1016 ORI

Authors
Citation
Ea. Vitrichenko, DUST ENVELOPES AROUND THE SECONDARY COMPONENTS OF BM ORI AND V1016 ORI, Astronomy letters, 24(5), 1998, pp. 611-622
Citations number
50
Categorie Soggetti
Astronomy & Astrophysics
Journal title
ISSN journal
10637737
Volume
24
Issue
5
Year of publication
1998
Pages
611 - 622
Database
ISI
SICI code
1063-7737(1998)24:5<611:DEATSC>2.0.ZU;2-#
Abstract
We explore the question of whether dust envelopes can survive around t he secondary components of the B stars BM Ori and V1016 Ori. The assum ption that such envelopes exist is shown to be unavoidable. Two altern ative compositions of these envelopes are considered: graphite and alp ha-cristobalite (alpha-SiO2, the refractory modification of quartz). F or the graphite envelope around the secondary of BM Ori, we have faile d to unambigously solve the question of its survival. The mean grain t emperature is below the graphite sublimation temperature. In the case of intense mixing, the envelope does not evaporate. If, however, the e nvelope is static (the case of corotation), then the dust temperature turns out to be lower than the sublimation temperature in 67% of the e nvelope and high in its remaining part (33%). The envelope then evapor ates. Model calculations show that 98% of the envelope does not evapor ate in: the case of grains coagulation, and, accordingly, it survives. Since the temperature of the entire quartz envelope is below the quar tz melting temperature, such an envelope can exist. An envelope made u p of graphite dust grains definitely cannot exist around the secondary of V1016 Ori-such dust evaporates. However, an envelope composed of q uartz grains can exist. In this case, quartz remains in a solid phase. We propose an observational check on the derived temperature distribu tion in the envelopes. To this end, we compare the temperatures and ra dii of the envelopes that we determined by analyzing the stars' contin uum in the bands from to M with those estimated from the dust-envelope models. The JHKL observations of deep minima in BM Ori also lend supp ort to the dust-envelope model. In the Appendix, we solve the light cu rve of V1016 Ori by assuming that the primary star is eclipsed both by the secondary and by the dust envelope. This solution is in satisfact ory agreement with the observations.