2005MNRAS.360..272L


Query : 2005MNRAS.360..272L

2005MNRAS.360..272L - Mon. Not. R. Astron. Soc., 360, 272-281 (2005/June-2)

Structure and evolution of low-mass W Ursae Majoris type systems - III. The effects of the spins of the stars.

LI L., HAN Z. and ZHANG F.

Abstract (from CDS):

In a previous paper, using Eggleton's stellar evolution code, we have discussed the structure and evolution of low-mass W Ursae Majoris (W UMa) type contact binaries with angular momentum loss owing to gravitational radiation or magnetic braking. We find that gravitational radiation is almost insignificant for cyclic evolution of low-mass W UMa type systems, and it is possible for angular momentum to be lost from W UMa systems in a magnetic stellar wind. The weaker magnetic activity shown by observations in W UMa systems is likely caused by the lower mass of the convective envelopes in these systems than in similar but non-contact binaries. The spin angular momentum cannot be neglected at any time for W UMa type systems, especially for those with extreme mass ratios. The spin angular momenta of both components are included in this paper and they are found to have a significant influence on the cyclic evolution of W UMa systems. We investigate the influence of the energy transfer on the common convective envelopes of both components in detail. We find that the mass of the convective envelope of the primary in contact evolution is slightly more than that in poor thermal contact evolution, and that the mass of the convective envelope of the secondary in contact evolution is much less than that in poor thermal contact evolution. Meanwhile, the rate of angular momentum loss of W UMa type systems is much lower than that of poor thermal contact systems. This is indeed caused by the lower masses of the convective envelopes of the components in W UMa type systems. Although the models with angular momentum loss for W UMa systems exhibit cyclic evolution, they seem to show that a W UMa system cannot continue this type of cyclic evolution indefinitely, and it might coalesce into a fast-rotating star after about 1200 cycles of evolution (about 7.0x109 yr).

Abstract Copyright: 2005 RAS

Journal keyword(s): stars: activity - binaries: close - stars: evolution - stars: rotation

Simbad objects: 6

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Number of rows : 6
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 V* EP Cep EB* 00 46 54.0135254616 +85 21 43.681861692 18.085 17.538 16.664 16.121 15.589 ~ 53 0
2 NGC 188 OpC 00 47 14.8 +85 14 42           ~ 990 0
3 V* EQ Cep EB* 00 47 33.3761816280 +85 16 24.254175108 18.521 17.547 16.703 16.142 15.951 ~ 59 0
4 V* ER Cep EB* 00 50 27.6907877016 +85 15 08.488920060 17.145 16.635 15.809 15.175 14.804 ~ 61 0
5 V* ES Cep EB* 00 50 50.0182856424 +85 16 11.720702352 16.864 16.549 15.872 15.188 15.048 ~ 60 0
6 V* FK Com PM* 13 30 46.7996390256 +24 13 57.781233768   9.04 8.245   7.204 G4III 384 1

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