A theory of hydrogen shell flashes on accreting white dwarfs. I - Their progress and the expansion of the envelope. II - The stable shell burning and the recurrence period of shell flashes
A theory of hydrogen shell flashes on accreting white dwarfs. I - Their progress and the expansion of the envelope. II - The stable shell burning and the recurrence period of shell flashes
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氢壳层理论闪现了吸积白矮星的现象。
DOI:
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发表时间:
1982
期刊:
影响因子:
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通讯作者:
M. Fujimoto
中科院分区:
文献类型:
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作者:
M. Fujimoto
By applying an analytical solution to the envelope, hydrogen shell flashes on accreting white dwarfs are computed semianlytically from their ignition to their final stage. When the mass of the white dwarf, M, and the mass of the hydrogen-rich envelope, ..delta..M/sub 1/, are specified, their progress is determined uniquely. Structural change and the resultant expansion of the envelope due to the shell flash depend mainly on the weight of overlying layer P(/sub 1/ or the product of the column mass above the burning shell and the surface gravity of the white dwarf. It is proved that this expansion is more rapid and greater for higher P(/sub 1/. When P(/sub 1/ is low (e.g.,< or approx. =4 x 10/sup 18/ dyn cm/sup -2/ for M = 1.0 M/sub sun/), the shell flash is weak, and the envelope settles in thermal equilibrium even before it expands to a solar radius. When P(/sub 1/ is high enough (10/sup 20/ dyn cm/sup -2/), on the other hand, the structural change is so violent that the expansion is accelerated beyond the escape velocity and leads directly to a nova explosion. Because of large P(/sub 1/, such a nova explosion requies a relatively large mass ofmore » the accreted envelope. The necessary mass of the envelope is as large as 10/sup -5/ M/sub sun/ even for white dwarfs close to the Chandrasekhar mass limit, and for less massive white dwarfs, it is still larger because of lower surface gravity. These results indicate that these nova explosions are phenomena which are related to surface gravity. These results indicate that these nova explosion are phenomena which are related to the slow accretion onto massive white dwarfs. Even for the optimal case of the most massive white dwarfs, the accretion rate should be lower than 10/sup -9/ M/sub sun/ yr/sup -1/.« less