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 - 2026
#notes
1 V* TW And SB* 00 03 18.2273024112 +32 50 45.105287892   9.48 9.07     F0/2V 140 0
2 V* TV Cas SB* 00 19 18.7425324624 +59 08 20.546623392 7.27 7.29 7.22     B9V 278 0
3 HD 5679 SB* 01 02 18.4439850768 +81 52 32.081564352   6.92 6.92     G2III:+B8/9 476 0
4 V* RY Per SB* 02 45 42.1225182912 +48 08 37.891142448   8.69 8.63     B4+F5III 160 0
5 V* RZ Cas SB* 02 48 55.5102370536 +69 38 03.441502644   6.40 6.26     A3V 471 0
6 * bet Per SB* 03 08 10.1324535 +40 57 20.328013 1.70 2.07 2.12 2.08 2.11 B8V 1265 1
7 V* AS Eri SB* 03 32 25.1263057224 -03 18 48.095135748   8.49 8.30     A3V+K0III 177 0
8 * lam Tau SB* 04 00 40.8167738514 +12 29 25.239987626 2.66 3.29 3.41 3.44 3.53 B4IV 364 0
9 V* RW Per SB* 04 20 16.7635224696 +42 18 51.812958564   10.19 9.72     A2 139 0
10 V* RS Cep SB* 05 06 03.2057646792 +80 14 52.280668284   10.76 10.39     A5III+G8III 105 0
11 V* IM Aur SB* 05 15 29.7441759312 +46 24 21.453397632   8.07 8.11     B7V 140 0
12 V* RX Gem SB* 06 50 11.5418579880 +33 14 20.728833000   9.42 9.24     A0+K2 92 0
13 HD 50846 SB* 06 54 54.7081653504 -01 22 32.850081768   8.44 8.43     B5/7Ib 162 0
14 V* R CMa SB* 07 19 28.1785241208 -16 23 42.895279824 6.09 6.05 5.70     F2III/IV 290 0
15 V* RY Gem SB* 07 27 24.1728227544 +15 39 34.699185396   8.88 8.68     A0V:e+K0II 151 0
16 V* TU Mon SB* 07 53 19.7486798832 -03 02 31.139762712   9.21 9.24     B2-6Vn 94 0
17 V* S Cnc SB* 08 43 56.1367272336 +19 02 03.038805888   8.44 8.35     B9/A0V+K:III 187 0
18 V* TX UMa SB* 10 45 20.5041244512 +45 33 58.708181052   6.99 6.98     B8V+G0III-IV 291 0
19 V* TT Hya SB* 11 13 12.4976326464 -26 27 54.253972800   7.43 7.31     F0IV:kA2mA3:_sh 193 0
20 * del Lib SB* 15 00 58.3483018872 -08 31 08.210408772 4.82 4.93 4.93 4.85 4.84 A0V 305 0
21 V* U CrB SB* 15 18 11.3524167096 +31 38 49.412401368   7.79 7.83     B6V 267 0
22 HD 139319 ** 15 33 51.05705 +63 54 25.6950           A9V+F7V 242 0
23 HD 139319A SB* 15 33 51.0591158448 +63 54 25.708209264   7.75 7.46     A5m 249 0
24 V* AI Dra SB* 16 56 18.1527589608 +52 41 54.348391608   7.18 7.13     A0V 186 0
25 V* RZ Sct SB* 18 26 33.5232714792 -09 12 05.987275200 8.09 8.24 7.53     B2/3Ib/II 176 0
26 V* KO Aql SB* 18 47 10.7415402480 +10 45 49.247482896   8.51 8.40     A0V 118 0
27 V* V356 Sgr SB* 18 47 52.3312296264 -20 16 28.243688340   7.07 6.99     B9III 179 0
28 HD 349425 SB* 18 50 00.3000055608 +20 43 16.509961596   10.08 9.72 9.77   A5 73 0
29 * U Sge SB* 19 18 48.4082723376 +19 36 37.722978540 6.23 6.61 6.58     B7III+K1III 385 0
30 V* Z Vul SB* 19 21 39.1059700488 +25 34 29.440304652 6.96 7.40 7.33     B3/5+A3IV? 213 0
31 V* V505 Sgr SB* 19 53 06.3860220576 -14 36 11.488005972   6.62 6.48     A2IV-V 213 0
32 V* WW Cyg SB* 20 04 02.7108881088 +41 35 16.462624380   10.163 10.10   9.875 B8k:+G? 118 0
33 V* SW Cyg SB* 20 06 57.9309043632 +46 17 58.151017284   9.57 9.35     A2 172 0
34 V* S Equ SB* 20 57 12.8405286120 +05 04 49.425738708   8.43 8.37     B8/9IV/V 132 1
35 V* AT Peg SB* 22 13 23.5161494184 +08 25 30.860613732   9.21 9.02     A6IV 119 0
36 V* Y Psc SB* 23 34 25.3846714008 +07 55 28.524147636   9.62 9.40     A3V+K0 111 0
37 V* XX Cep SB* 23 38 20.2850614704 +64 20 02.699063196   9.47 9.18     A7V 165 0

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