The Breakout of Protostellar Winds in the Infalling Environment

dc.creatorWilkin, Francis P.
dc.date2002-11-26
dc.date.accessioned2026-07-07T02:06:34Z
dc.date.available2026-07-07T02:06:34Z
dc.descriptionThe time of protostellar wind breakout may be determined by the evolution of the infalling flow, rather than any sudden change in the central engine. I examine the transition from pure infall to outflow, in the context of the inside-out collapse of a rotating molecular cloud core. I have followed numerically the motion of the shocked shell created by the impact of a stellar wind and infalling gas. These fully time-dependent calculations include cases both where the shell falls back to the stellar surface, and where it breaks out as a true outflow. Assuming a wind launched from the protostellar surface, the breakout time is determined in terms of the parameters describing the wind (Mdot_w, V_w) and collapsing cloud core (a_0, Omega). The trapped wind phase consists of a wind sufficiently strong to push material back from the stellar surface, but too weak to carry the heavy, shocked infall out of the star's gravitational potential. To produce a large-scale outflow, the shocked material must be able to climb out of the star's gravitational potential well, carrying with it the dense, swept-up infall.
dc.description5 Pages, Proceedings of "The Interaction of Stars with their Environment II", Budapest, Hungary May 15-18, 2002
dc.identifierhttps://arxiv.org/abs/astro-ph/0211583
dc.identifierhttp://arxiv.org/abs/astro-ph/0211583
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/5405
dc.subjectAstrophysics
dc.titleThe Breakout of Protostellar Winds in the Infalling Environment
dc.typetext

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