Why a New Code for Novae Evolution and Mass Transfer in Binaries?

One of the most interesting problems in Cataclysmic Variables is the long time scale evolution. This problem appears in long time evolution, which is also very important in the search for the progenitor of SN Ia. The classical approach to overcome this problem in the simulation of novae evolution is...

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Main Authors: G. Shaviv, I. Idan, N. J. Shaviv
Format: Article
Language:English
Published: CTU Central Library 2015-02-01
Series:Acta Polytechnica CTU Proceedings
Online Access:https://ojs.cvut.cz/ojs/index.php/APP/article/view/2849
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spelling doaj-7c368d23aa07497f999d225d51be35b32020-11-24T22:29:04ZengCTU Central LibraryActa Polytechnica CTU Proceedings2336-53822015-02-012110310610.14311/APP.2015.02.01032617Why a New Code for Novae Evolution and Mass Transfer in Binaries?G. Shaviv0I. Idan1N. J. Shaviv2Department of Physics, Israel Institute of Technology, Haifa, IsraelDepartment of Physics, Israel Institute of Technology, Haifa, IsraelRacah Institute of Physics, The Hebrew University, Jerusalem, IsraelOne of the most interesting problems in Cataclysmic Variables is the long time scale evolution. This problem appears in long time evolution, which is also very important in the search for the progenitor of SN Ia. The classical approach to overcome this problem in the simulation of novae evolution is to assume: (1) A constant in time, rate of mass transfer. (2) The mass transfer rate that does not vary throughout the life time of the nova, even when many eruptions are considered. Here we show that these assumptions are valid only for a single thermonuclear flash and such a calculation cannot be the basis for extrapolation of the behavior over many flashes. In particular, such calculation cannot be used to predict under what conditions an accreting WD may reach the Chandrasekhar mass and collapse. We report on a new code to attack this problem. The basic idea is to create two parallel processes, one calculating the mass losing star and the other the accreting white dwarf. The two processes communicate continuously with each other and follow the time depended mass loss.https://ojs.cvut.cz/ojs/index.php/APP/article/view/2849
collection DOAJ
language English
format Article
sources DOAJ
author G. Shaviv
I. Idan
N. J. Shaviv
spellingShingle G. Shaviv
I. Idan
N. J. Shaviv
Why a New Code for Novae Evolution and Mass Transfer in Binaries?
Acta Polytechnica CTU Proceedings
author_facet G. Shaviv
I. Idan
N. J. Shaviv
author_sort G. Shaviv
title Why a New Code for Novae Evolution and Mass Transfer in Binaries?
title_short Why a New Code for Novae Evolution and Mass Transfer in Binaries?
title_full Why a New Code for Novae Evolution and Mass Transfer in Binaries?
title_fullStr Why a New Code for Novae Evolution and Mass Transfer in Binaries?
title_full_unstemmed Why a New Code for Novae Evolution and Mass Transfer in Binaries?
title_sort why a new code for novae evolution and mass transfer in binaries?
publisher CTU Central Library
series Acta Polytechnica CTU Proceedings
issn 2336-5382
publishDate 2015-02-01
description One of the most interesting problems in Cataclysmic Variables is the long time scale evolution. This problem appears in long time evolution, which is also very important in the search for the progenitor of SN Ia. The classical approach to overcome this problem in the simulation of novae evolution is to assume: (1) A constant in time, rate of mass transfer. (2) The mass transfer rate that does not vary throughout the life time of the nova, even when many eruptions are considered. Here we show that these assumptions are valid only for a single thermonuclear flash and such a calculation cannot be the basis for extrapolation of the behavior over many flashes. In particular, such calculation cannot be used to predict under what conditions an accreting WD may reach the Chandrasekhar mass and collapse. We report on a new code to attack this problem. The basic idea is to create two parallel processes, one calculating the mass losing star and the other the accreting white dwarf. The two processes communicate continuously with each other and follow the time depended mass loss.
url https://ojs.cvut.cz/ojs/index.php/APP/article/view/2849
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