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From: David A. <wda...@gm...> - 2014-01-14 19:17:51
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1. The He abundance is not known to that accuracy (0.2447). By slightly adjusting it (less He, so more opacity) you can get L to fit the observed value. 2. Both Teff and Rcz depend upon the convective model. At present MESA uses mixing-length theory in a one-parameter form. That parameter is the mixing-length alpha, and it is adjusted to fix the radius (Teff plus L). 3. This leaves us no further adjustments to fit the helio-seismological data (Rcz), except for the metalicity. The conventional conclusion is that the Asplund metalicity is too low because of the above discrepancy with Rcz. An alternative possibility is that mixing-length theory is not accurate enough. For example, it ignores Reynolds stresses, an error that must be absorbed by the choice of alpha; it is not obvious that this is the same physics that determines the deep convection at the lower boundary (Rcz). This, or some other aspect of turbulent convection not included in mixing-length theory, may be the root of the problem. Look at http://www.nasa.gov/mission_pages/sdo/news/coronal-rain.html and see if you thinks a one-parameter model fits solar convection ;-) I am inclined to the view that the Asplund abundances are correct and the stellar models are wrong, but that is just my opinion. Don't forget, the models are not so VERY wrong even with MLT. I hope this helps. -- David Arnett Regents Professor Steward Observatory University of Arizona Facts are stubborn, but statistics are more pliable. Mark Twain Facts do not cease to exist because they are ignored. Aldous Huxley |