1975
DOI: 10.1086/153675
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P Cygni stars and mass loss

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Cited by 33 publications
(15 citation statements)
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“…The problem of multiple-branched equal velocity surfaces is known from modeling of line profiles from decelerating atmospheres ( Kuan & Kuhi (1975), Surdej (1977). These authors adopted a decelerating velocity law, v(r) = V const (R ph /r) l , where l > 0 is a parameter of deceleration and R ph is the radius of the photosphere.…”
Section: Optical Depthmentioning
confidence: 99%
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“…The problem of multiple-branched equal velocity surfaces is known from modeling of line profiles from decelerating atmospheres ( Kuan & Kuhi (1975), Surdej (1977). These authors adopted a decelerating velocity law, v(r) = V const (R ph /r) l , where l > 0 is a parameter of deceleration and R ph is the radius of the photosphere.…”
Section: Optical Depthmentioning
confidence: 99%
“…Another approximate approach was adopted by Kuan & Kuhi (1975) who ignored the radiative coupling between s and s ′ . In the literature this is known as the 'disconnected approximation' ( Marti & Noerdlinger (1977)).…”
Section: Radiation Field In a Linementioning
confidence: 99%
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“…For application we use the prototype of LBVs, P Cyg, as the central star following Paper I. The envelope of this star may possess a deceleration region (Kuan & Kuhi 1975;Nugis et al 1979) and also exhibits shells or blobs (Vakili et al 1997). These outflows may not arise as thick-line-driven winds but from the absorption of a large number of the weak, optically thin spectral UV lines in the Balmer continuum (Lamers 1986).…”
Section: The Energetics Of Steady Shell Thermo-radiative Casementioning
confidence: 99%
“…By contrast, the strong winds observed in early main-sequence stars are traditionally modeled by the thick-line-driven wind theory (Castor et al 1975) which is based on the Sobolev approximation. However, the reduced acceleration near the stellar surface and the low terminal velocity of winds from supergiants cannot be accounted for thick-line driving (as for example has been extensively discussed by Lamers (1986) for P Cyg), as well as the possible deceleration regions in the stellar envelope (Kuan & Kuhi 1975). Assuming e-mail: akakour@cc.uoa.gr an optically thin stellar atmosphere, Kakouris & Moussas (1998), hereafter Paper I, proposed an alternative thermoradiative mechanism which can describe the deceleration region in the stellar envelope and steady shell formation under certain conditions.…”
Section: Introductionmentioning
confidence: 99%