2000A&A...360..969R


Query : 2000A&A...360..969R

2000A&A...360..969R - Astronomy and Astrophysics, volume 360969-990 (2000/8-3)

Irradiation and mass transfer in low-mass compact binaries.

RITTER H., ZHANG Z.-Y. and KOLB U.

Abstract (from CDS):

This paper studies the reaction of low-mass stars to anisotropic irradiation and its implications for the long-term evolution of compact binaries (cataclysmic variables and low-mass X-ray binaries). First, we show by means of simple homology considerations that if the energy outflow through the surface layers of a low-mass main sequence star is blocked over a fraction seff<1 of its surface (e.g. as a consequence of anisotropic irradiation) it will inflate only modestly, by a factor ~(1-seff)–0.1. The maximum contribution to mass transfer of the thermal relaxation of the donor star is seff times what one obtains for isotropic (seff=1) irradiation. The duration of this irradiation-enhanced mass transfer is of the order of 0.1|ln((1-s)eff)| times the thermal time scale of the convective envelope. Numerical computations involving full 1D stellar models confirm these results. Second, we present a simple analytic one-zone model for computing the blocking effect by irradiation which gives results in acceptable quantitative agreement with detailed numerical computations. Third, we show in a detailed stability analysis that if mass transfer is not strongly enhanced by consequential angular momentum losses, cataclysmic variables are stable against irradiation-induced runaway mass transfer if the mass of the main sequence donor is M≲0.7M☉. If M>0.7M☉ systems may be unstable, subject to the efficiency of irradiation. Low-mass X-ray binaries, despite providing much higher irradiating fluxes, are even less susceptible to this instability. If a binary is unstable, mass transfer must evolve through a limit cycle in which phases of irradiation-induced high mass transfer alternate with phases of small (or no) mass transfer. At the peak rate mass transfer proceeds on seff times the thermal time scale rate of the convective envelope. A necessary condition for the cycles to be maintained is that this time scale has to be much shorter (≲0.05) than the time scale on which mass transfer is driven.

Abstract Copyright: ∼

Journal keyword(s): accretion, accretion disks - stars: binaries: close - stars: evolution - stars: interiors - stars: novae, cataclysmic variables - X-rays: stars

Simbad objects: 14

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Number of rows : 14
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 PN HFG 1 PN 03 03 47.0096763024 +64 54 35.517676320     14.56 13.99   ~ 114 0
2 HD 269696 HS* 05 31 40.3594532592 -69 53 02.153902236 9.74 10.92 11.15     sdB+dM 202 0
3 PN K 1-2 PN 08 57 45.9621412752 -28 57 36.577846476           ~ 125 1
4 CD-48 6027 HS* 10 54 40.5601100160 -48 47 02.815818036 10.92 11.99 12.12 12.39   sdO 127 0
5 V* BE UMa CV* 11 57 44.8279856952 +48 56 18.313757772   15.437 15.373 14.867   DO+M1/5e 140 0
6 EC 11575-1845 HS* 12 00 05.6456553960 -19 02 03.968781864   13.02 13.20 13.51   sdO+dMe 41 1
7 BD-07 3477 HS* 12 44 20.2386233232 -08 40 16.846099536   10.46 10.594 10.895   sdB2VIIHe3 303 1
8 HD 126719 ** 14 26 02.3823688239 +42 13 05.147831632   9.54 8.89     G5 34 0
9 V* NN Ser RS* 15 52 56.1203524080 +12 54 44.429312196     16.51     DAO1+M4 287 0
10 PN A66 41 PN 17 29 02.0258857104 -15 13 04.482114960   16.06 15.95     sdO 146 1
11 BD+27 2853 ** 17 37 10.7609846 +27 53 47.116940   10.35 9.22 9.039   K5 86 0
12 PN A66 46 PN 18 31 18.5910709560 +26 56 12.110750088       15.050   O9k 190 0
13 PN A66 63 PN 19 42 10.2896588688 +17 05 14.458509132           sdO+G: 222 1
14 GD 245 CV* 22 58 48.1351624092 +25 15 43.908615894   13.699 13.650 13.833   DA2.2 74 0

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