2010MNRAS.406.1071D


Query : 2010MNRAS.406.1071D

2010MNRAS.406.1071D - Mon. Not. R. Astron. Soc., 406, 1071-1083 (2010/August-1)

Spin angular momentum evolution of the long-period Algols.

DERVISOGLU A., TOUT C.A. and IBANOGLU C.

Abstract (from CDS):

We consider the spin angular momentum evolution of the accreting components of Algol-type binary stars. In wider Algols the accretion is through a disc so that the accreted material can transfer enough angular momentum to the gainer that material at its equator should be spinning at breakup. We demonstrate that even a small amount of mass transfer, much less than required to produce today's mass ratios, transfers enough angular momentum to spin the gainer up to this critical rotation velocity. However the accretors in these systems have spins typically between 10 and 40per cent of the critical rate. So some mechanism for angular momentum loss from the gainers is required. Unlike solar-type chromospherically active stars, with enhanced magnetic activity which leads to angular momentum and mass loss, the gainers in classical Algols have radiative envelopes. We further find that normal radiative tides are far too weak to account for the necessary angular momentum loss. Thus enhanced mass loss in a stellar wind seems to be required to spin-down the gainers in classical Algol systems. We consider generation of magnetic fields in the radiative atmospheres in a differentially rotating star and the possibility of angular momentum loss driven by strong stellar winds in the intermediate-mass stars, such as the primaries of the Algols. Differential rotation, induced by the accretion itself, may produce such winds which carry away enough angular momentum to reduce their rotational velocities to the today's observed values. We apply this model to two systems with initial periods of 5d, one with initial masses 5 and and the other with 3.2 and. Our calculations show that, if the mass outflow rate in the stellar wind is about 10per cent of the accretion rate and the dipole magnetic field is stronger than about 1kG, the spin rate of the gainer is reduced to below breakup velocity even in the fast phase of mass transfer. Larger mass loss is needed for smaller magnetic fields. The slow rotation of the gainers in the classical Algol systems is explained by a balance between the spin-up by mass accretion and spin-down by a stellar wind linked to a magnetic field.

Abstract Copyright: © 2010 The Authors. Journal compilation © 2010 RAS

Journal keyword(s): binaries: close - stars: evolution - stars: magnetic fields - stars: winds, outflows

Simbad objects: 37

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Number of rows : 37
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 V* TW And EB* 00 03 18.2273024112 +32 50 45.105287892   9.48 9.07     F0/2V 136 0
2 V* TV Cas EB* 00 19 18.7425324624 +59 08 20.546623392 7.27 7.29 7.22     B9V 271 0
3 V* U Cep EB* 01 02 18.4439850768 +81 52 32.081564352   6.92 6.92     G2III:+B8/9 467 0
4 V* RY Per EB* 02 45 42.1225182912 +48 08 37.891142448   8.69 8.63     B4+F5III 153 0
5 V* RZ Cas EB* 02 48 55.5102370536 +69 38 03.441502644   6.40 6.26     A3V 456 0
6 * bet Per EB* 03 08 10.1324535 +40 57 20.328013 1.70 2.07 2.12 2.08 2.11 B8V 1219 1
7 V* AS Eri EB* 03 32 25.1263057224 -03 18 48.095135748   8.49 8.30     A3V+K0III 172 0
8 * lam Tau EB* 04 00 40.8167738514 +12 29 25.239987626 2.66 3.29 3.41 3.44 3.53 B4IV 349 0
9 V* RW Per EB* 04 20 16.7635224696 +42 18 51.812958564   10.19 9.72     A2 135 0
10 V* RS Cep EB* 05 06 03.2057646792 +80 14 52.280668284   10.76 10.39     A5III+G8III 102 0
11 V* IM Aur EB* 05 15 29.7441759312 +46 24 21.453397632   8.07 8.11     B7V 133 0
12 V* RX Gem EB* 06 50 11.5418579880 +33 14 20.728833000   9.42 9.24     A0+K2 88 0
13 HD 50846 EB* 06 54 54.7081653504 -01 22 32.850081768   8.46 8.43     B5/7Ib 149 0
14 V* R CMa EB* 07 19 28.1785241208 -16 23 42.895279824 6.09 6.05 5.70     F2III/IV 282 0
15 V* RY Gem EB* 07 27 24.1728227544 +15 39 34.699185396   8.88 8.68     A0V:e+K0II 145 0
16 V* TU Mon EB* 07 53 19.7486798832 -03 02 31.139762712   9.21 9.24     B2-6Vn 90 0
17 V* S Cnc EB* 08 43 56.1367272336 +19 02 03.038805888   8.44 8.35     B9/A0V+K:III 184 0
18 V* TX UMa EB* 10 45 20.5041244512 +45 33 58.708181052   6.99 6.98     B8V+G0III-IV 282 0
19 V* TT Hya EB* 11 13 12.4976326464 -26 27 54.253972800   7.43 7.31     F0IV:kA2mA3:_sh 188 0
20 * del Lib EB* 15 00 58.3483018872 -08 31 08.210408772 4.82 4.93 4.93 4.85 4.84 A0V 293 0
21 V* U CrB EB* 15 18 11.3524167096 +31 38 49.412401368   7.79 7.83     B6V 260 0
22 HD 139319 EB* 15 33 51.05705 +63 54 25.6950           ~ 239 0
23 HD 139319A SB* 15 33 51.0591158448 +63 54 25.708209264   7.75 7.46     A5m 247 0
24 V* AI Dra EB* 16 56 18.1527589608 +52 41 54.348391608   7.18 7.13     A0V 181 0
25 V* RZ Sct EB* 18 26 33.5232714792 -09 12 05.987275200 8.09 8.24 7.53     B2/3Ib/II 170 0
26 V* KO Aql EB* 18 47 10.7415402480 +10 45 49.247482896   8.51 8.40     A0V 117 0
27 V* V356 Sgr EB* 18 47 52.3312296264 -20 16 28.243688340   7.07 6.99     B9III 173 0
28 HD 349425 EB* 18 50 00.3000055608 +20 43 16.509961596   10.08 9.72 9.77   A5 71 0
29 * U Sge EB* 19 18 48.4082723376 +19 36 37.722978540 6.23 6.61 6.58     B7III+K1III 373 0
30 V* Z Vul EB* 19 21 39.1059700488 +25 34 29.440304652 6.96 7.40 7.33     B3/5+A3IV? 207 0
31 V* V505 Sgr EB* 19 53 06.3860220576 -14 36 11.488005972   6.62 6.48     A2IV-V 207 0
32 V* WW Cyg EB* 20 04 02.7108881088 +41 35 16.462624380   10.163 10.10   9.875 B8k:+G? 113 0
33 V* SW Cyg EB* 20 06 57.9309043632 +46 17 58.151017284   9.57 9.35     A2 166 0
34 V* S Equ EB* 20 57 12.8405286120 +05 04 49.425738708   8.43 8.37     B8/9IV/V 130 1
35 V* AT Peg EB* 22 13 23.5161494184 +08 25 30.860613732   9.21 9.02     A6IV 113 0
36 V* Y Psc EB* 23 34 25.3846714008 +07 55 28.524147636   9.62 9.40     A3V+K0 107 0
37 V* XX Cep SB* 23 38 20.2850614704 +64 20 02.699063196   9.47 9.18     A7V 161 0

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