2002A&A...388..518C


Query : 2002A&A...388..518C

2002A&A...388..518C - Astronomy and Astrophysics, volume 388518-530 (2002/6-3)

New results on the apsidal-motion test to stellar structure and evolution including the effects of dynamic tides.

CLARET A. and WILLEMS B.

Abstract (from CDS):

We revised the current status of the apsidal-motion test to stellar structure and evolution. The observational sample was increased by about 50% in comparison to previous studies. Classical and relativistic systems were analyzed simultaneously and only systems with accurate absolute dimensions were considered. New interior models incorporating recent opacity tables, stellar rotation, mass loss, and moderate core overshooting were used as theoretical tools to compare the predicted with the observed shifts of the position of the periastron. The stellar models were computed for the precise observed masses and the adopted chemical compositions are consistent with the corresponding tables of opacities to avoid the inherent problems of interpolation in mass and in (X, Z). The derived chemical composition for each individual system was used to infer the primordial helium content as well as a law of enrichment. The values found are in good agreement with those obtained from various independent sources. For the first time, the effects of dynamic tides are taken into account systematically to determine the contribution of the tidal distortion to the predicted apsidal-motion rate. The deviations between the apsidal-motion rates resulting from the classical formula and those determined by taking into account the effects of dynamic tides are presented as a function of the level of synchronism. For systems close to synchronisation, dynamic tides cause deviations with respect to the classical apsidal-motion formula due to the effects of the compressibility of the stellar fluid. For systems with higher rotational angular velocities, additional deviations due to resonances arise when the forcing frequencies of the dynamic tides come into the range of the free oscillation modes of the component stars. The resulting comparison shows a good agreement between the observed and theoretical apsidal-motion rates. No systematic effects in the sense that models are less mass concentrated than real stars and no correlations with the evolutionary status of the systems were detected.

Abstract Copyright: ∼

Journal keyword(s): stars: binaries: close - stars: evolution - stars: interiors - stars: oscillations - stars: abundances

Simbad objects: 39

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Number of rows : 39
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 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 13622 1
2 * 21 Cas SB* 00 45 39.0765692400 +74 59 17.054172672   5.717 5.652     A2IV 222 0
3 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
4 * zet Phe SB* 01 08 23.0805843521 -55 14 44.736015873   3.908 4.014     B6V+B9V 243 0
5 V* AI Phe SB* 01 09 34.1924055096 -46 15 56.071719360   9.26 8.60     F7V+K0IV 157 0
6 V* IQ Per SB* 03 59 44.6764997640 +48 09 04.487282712   7.77 7.73     B9 162 0
7 HD 25833A SB* 04 06 55.8286148575 +33 26 46.929071509   6.83 6.87     ~ 264 0
8 HD 25833 ** 04 06 55.8351101323 +33 26 47.009585515       7.71   B3Vn 269 0
9 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
10 * 31 Men SB* 05 30 13.8827476176 -84 47 06.365764140   6.169 6.186     B9.5IV/V 138 0
11 V* GG Ori SB* 05 43 10.2226873248 -00 41 14.798359644   10.92       A2 79 0
12 HD 38735 SB* 05 47 26.8930346587 -10 31 58.690687745   6.23 6.09     A2IV 123 0
13 V* GZ CMa SB* 07 16 19.2051179904 -16 43 00.074716140   8.14 7.98     A0III/IV 73 0
14 V* AI Hya EB* 08 18 47.4972221712 +00 17 00.612058128   9.77 9.35     F2m+F0V 119 0
15 V* V596 Pup SB* 08 27 33.2749537514 -20 50 38.246097199   6.63 6.59     A1V 123 1
16 * 163 Car SB* 09 54 33.8842758792 -58 25 16.579713612 5.6 6.47 6.64     B2V 128 0
17 V* HS Hya SB* 10 24 36.7678198944 -19 05 32.956244232   8.55 8.10     F5V 123 0
18 V* EM Car SB* 11 12 04.5060592584 -61 05 42.944560584 8.06 8.80 8.54 9.25   O7.5V((f))+O7.5V((f)) 172 0
19 * alf Vir bC* 13 25 11.57937 -11 09 40.7501 -0.20 0.74 0.97 1.06 1.30 B1V 877 1
20 V* GG Lup SB* 15 18 56.3746551072 -40 47 17.596548564   5.495 5.604 5.613   B7V 146 0
21 V* V760 Sco SB* 16 24 43.7182304928 -34 53 37.529154204   7.16 7.05     B4V 176 0
22 V* U Oph SB* 17 16 31.7137908168 +01 12 37.998551304   5.941 5.921     B3V 388 1
23 V* V539 Ara SB* 17 50 28.3930000656 -53 36 44.664776352   5.60 5.71     B2/3Vnn 190 0
24 HD 163708 SB* 17 59 13.4703104784 -36 56 19.839700356   7.155 7.089 8.09   A3III 122 0
25 V* V451 Oph SB* 18 29 14.0426779320 +10 53 31.429623012   7.95 7.91     A0IV 167 0
26 V* DI Her SB* 18 53 26.2399243224 +24 16 40.792648332   8.46 8.47     B5III 274 0
27 V* V1143 Cyg SB* 19 38 41.1829269072 +54 58 25.647010572       5.6   F6Va 229 0
28 V* V1765 Cyg SB* 19 48 50.5979466384 +33 26 14.222537016 5.99 6.578 6.463     B0.5II 151 0
29 V* V380 Cyg SB* 19 50 37.3267754400 +40 35 59.135141652 4.86 5.613 5.680     B1.1III+B2.5/3V: 305 0
30 V* V477 Cyg SB* 20 05 27.6886714176 +31 58 18.108420780   8.68 8.53     A1V 219 0
31 V* Y Cyg SB* 20 52 03.5771840640 +34 39 27.486121104 6.31 7.23 7.32     O9.5IV+O9.5IV 382 0
32 V* EE Peg SB* 21 40 01.8804448032 +09 11 05.150643900   7.08 6.96     A1III 172 0
33 V* EK Cep SB* 21 41 21.5042268336 +69 41 34.112933916   7.95 7.89     A0V 222 0
34 V* BW Aqr SB* 22 23 15.9305850720 -15 19 56.201783268   10.8 10.3     F7 114 0
35 V* WX Cep SB* 22 31 15.7881709512 +63 31 21.554196312   9.38 9.00     A5V+A2V 112 0
36 V* V364 Lac SB* 22 52 14.8100362992 +38 44 44.634368292   8.54 8.36     A4m+A3m 101 0
37 HD 218066 Be* 23 04 02.2270838832 +63 23 48.722060508 7.50 7.97 7.6     B1.5Vn 290 0
38 V* PV Cas SB* 23 10 02.5750345872 +59 12 06.149248560   9.98 9.86     B6V 159 0
39 V* IT Cas SB* 23 42 01.3774276248 +51 44 36.818206584   11.57 11.23     F6 76 0

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