Hostname: page-component-76fb5796d-22dnz Total loading time: 0 Render date: 2024-04-26T21:57:35.183Z Has data issue: false hasContentIssue false

Definitions, Summary, and Some Issues

Published online by Cambridge University Press:  30 March 2016

Peter S. Conti*
Affiliation:
JILA and APS Department, University of Colorado, Boulder CO 80309

Extract

Core share and HTML view are not available for this content. However, as you have access to this content, a full PDF is available via the ‘Save PDF’ action button.

This Joint Discussion has been titled Massive Star Birth. Perhaps it is appropriate here to define what we mean by a massive star. The very word massive suggests we consider a minimum mass M below which one would speak of low (or intermediate) mass evolution, and above which is the realm of massive stars. It is natural to take this mass limit as that in which a (single) star will end its life as a supernova: 8M. This corresponds to a (minimum) luminosity L of a few × 103L, a (minimum) Teff of 20000 K, and a ZAMS spectral type of about B1.5V. Note that this mass division refers to the final evolution of a star, and might well have nothing to do with difference in physical processes between massive and low mass star birth. For example, the minimum Teff for a star to produce an UCHII region, a readily observable quantity, corresponds to a Teff closer to 30000 K and a mass of 15M.

Type
II. Joint Discussions
Copyright
Copyright © Astronomical Society of Pacific 2002