1981
DOI: 10.1093/mnras/194.4.967
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The evolution of viscous discs - I. Mass transfer variations

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Cited by 140 publications
(85 citation statements)
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“…The model by Bath & Pringle (1981) shows that both the disk luminosity and structure settle down in a time considerably shorter than the observed main outburst. The observed very slow decay can be explained if the mass inflow rate from the donor to the disk,ṁ tr , becomes a significant fraction of the mass accretion rate from the disk onto the NS,ṁ acc during the outburst (Eq.…”
Section: Discussionmentioning
confidence: 92%
“…The model by Bath & Pringle (1981) shows that both the disk luminosity and structure settle down in a time considerably shorter than the observed main outburst. The observed very slow decay can be explained if the mass inflow rate from the donor to the disk,ṁ tr , becomes a significant fraction of the mass accretion rate from the disk onto the NS,ṁ acc during the outburst (Eq.…”
Section: Discussionmentioning
confidence: 92%
“…For this computation we have taken Rmin = 5AU and Rmax = 1056AU. We use a radial grid of 400 points equally spaced in √ R (Bath & Pringle 1981). At time t = 0, mass is injected steadily and the number density starts growing, creating a spike around 85AU.…”
Section: Evolution To the Steady State Of An α Disc With Fixed Tempermentioning
confidence: 99%
“…To calculateK we replaced in relation (5) R g by R disk and T eff, g by T edge, disk , using relations (A.2) and (A.3). The characteristic disk temperature and the temperature distribution from the stellar surface to the edge of the disk were calculated from the model of Bath & Pringle (1981). Horne (1985) developed a method of eclipse mapping of accretion disks with this model, and Rutten et al (1992) applied the latter method to construct models of accretion disks for six cataclysmic variables.…”
Section: A2 Three Gainers With An Accretion Diskmentioning
confidence: 99%