User:Tohline/Appendix/Ramblings/OriginOfPlanetaryNebulae

From VistrailsWiki
< User:Tohline‎ | Appendix/Ramblings
Revision as of 05:23, 20 November 2016 by Tohline (talk | contribs) (Created page with '<!-- __FORCETOC__ will force the creation of a Table of Contents --> <!-- __NOTOC__ will force TOC off --> =On the Origin of Planetary Nebulae= This chapter — initially cre…')
(diff) ← Older revision | Latest revision (diff) | Newer revision → (diff)
Jump to navigation Jump to search

On the Origin of Planetary Nebulae

This chapter — initially created by J. E. Tohline on 19 November 2016 — is intended primarily to provide a summary of the research that has been undertaken following a discussion that took place on 3 July 2013 with Kundan Kadam (an LSU graduate student, at the time) regarding the stability of bipolytropes.


Whitworth's (1981) Isothermal Free-Energy Surface
|   Tiled Menu   |   Tables of Content   |  Banner Video   |  Tohline Home Page   |

Context

Why do stars become red giants? In particular, why does a star on the main sequence — whose internal density profile is only moderately centrally concentrated — readjust it internal structure to become a red giant — which has a highly centrally condensed structure — at the end of the core-hydrogen-burning phase of its evolution? It seems likely that this evolutionary transition is triggered by an instability associated with the Schönberg-Chandrasekhar mass limit. The inert helium core that is "left behind" is approximately isothermal — because the helium, itself, is not hot enough to burn — and this is not good from a structural or stability standpoint because self-gravitating, isothermal structures are notoriously unstable. Henrich & Chandraskhar (1941) and Schönberg & Chandrasekhar (1942)) discovered that a star with an isothermal core will become unstable if the fractional mass of the core is above some limiting value.

Treating as bipolytrope with <math>~(n_c, n_e) = (\infty, 3/2)</math> SC showed that this evolution is accompanied by a structural change toward a more centrally condensed structure. Faulkner et al. showed this more cleanly with analytic bipolytropic structures with <math>~(n_c, n_e) = (5, 1)</math>. We wondered whether mass-transfer in a binary system might accelerate the process. What type of instability results from exceeding the SC mass limit? Is it secular, or might it be dynamical? And what is the consequence; does the core collapse on a dynamical time scale; or does the envelope get "kicked off" to form a planetary nebula; or both?


See Also

Whitworth's (1981) Isothermal Free-Energy Surface

© 2014 - 2021 by Joel E. Tohline
|   H_Book Home   |   YouTube   |
Appendices: | Equations | Variables | References | Ramblings | Images | myphys.lsu | ADS |
Recommended citation:   Tohline, Joel E. (2021), The Structure, Stability, & Dynamics of Self-Gravitating Fluids, a (MediaWiki-based) Vistrails.org publication, https://www.vistrails.org/index.php/User:Tohline/citation