1976
DOI: 10.1086/154840
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An infall model for the T Tauri phenomenon

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Cited by 341 publications
(359 citation statements)
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“…For this purpose, they used a detailed emission model, coupled with an analytical model for the envelope, the cavity, and the disk. The envelope model is that of a rotating, collapsing sphere developed by Ulrich (1976), with a cavity in which the density is set to zero to mimic the outflows. The disk density is given by a power-law dependence in radius and a Gaussian dependence in height (see Enoch et al (2009) for more details).…”
Section: Comparison With Observationsmentioning
confidence: 99%
“…For this purpose, they used a detailed emission model, coupled with an analytical model for the envelope, the cavity, and the disk. The envelope model is that of a rotating, collapsing sphere developed by Ulrich (1976), with a cavity in which the density is set to zero to mimic the outflows. The disk density is given by a power-law dependence in radius and a Gaussian dependence in height (see Enoch et al (2009) for more details).…”
Section: Comparison With Observationsmentioning
confidence: 99%
“…For the model of the envelope structure we follow the ideas of Ulrich (1976). We thus implement a model for a rotating envelope resulting from infalling matter similar to Whitney et al (2003); Eisner et al (2005):…”
Section: The Envelopementioning
confidence: 99%
“…As is predicted from the present star formation theories, lowmass star models have an infalling envelope at a large distance from the central star and a rotating disk inside the envelope (Shakura & Sunyaev 1973;Ulrich 1976;Cassen & Moosman 1981;Pringle 1981;Terebey et al 1984). We assume a form that is often used in T Tauri models, and the mass density distribution ρ is given by…”
Section: Model Assumptionmentioning
confidence: 99%