2003MNRAS.342.1260Q


Query : 2003MNRAS.342.1260Q

2003MNRAS.342.1260Q - Mon. Not. R. Astron. Soc., 342, 1260-1270 (2003/July-2)

Are overcontact binaries undergoing thermal relaxation oscillation with variable angular momentum loss.

QIAN S.

Abstract (from CDS):

Orbital period variations of five W-type overcontact binaries, GW Cep, VY Cet, V700 Cyg, EM Lac and AW Vir, are presented based on the analysis of all available times of light minimum. It is discovered that the period of GW Cep is decreasing at a rate of dP/dt =-6.62 x10–8 d/yr. For VY Cet and V700 Cyg, a cyclic oscillation is found superimposed on a secular period increase, which can be explained either by the light-time effect of an assumed third body or by magnetic activity cycles. For the other two, EM Lac and AW Vir, the periods show a secular increase. GW Cep is a low mass ratio system with q = 0.37, while the others are high mass ratio systems (q = 0.67, 0.65, 0.63 and 0.76, respectively). The period changes of the five sample stars are in good agreement with Qian's conclusion that low mass ratio overcontact binaries usually show a decreasing period, while the periods of high mass ratio systems are increasing.

Based on the period variations of 59 overcontact binaries, a statistical investigation of period change is given. It is confirmed that the period change of a W UMa-type binary star is correlated with the mass ratio (q) and with the mass of the primary component (M1). Meanwhile, some statistical relations (M1-P, Js-M1, J s-M2and Js-P) for overcontact binaries are presented using the absolute parameters of 78 systems. From these relations, the following results may be drawn: (i) free mass transfer in both directions exists between the components, which is assumed by thermal relaxation oscillation (TRO) theory; (ii) angular momentum loss (AML) can make a W UMa-type star maintain shallow overcontact and not evolve from overcontact to semidetached configurations as proposed by Rahunen; (iii) the evolution of the W UMa-type systems may be oscillation around a critical mass ratio, while the critical mass ratio varies with the mass of the primary component. These results can be plausibly explained by the combination of the TRO and the variable AML via a change of depth of the overcontact, which is consistent with the X-ray and IUE observations.


Abstract Copyright: 2003 RAS

Journal keyword(s): binaries: close - stars: evolution - stars: magnetic fields - stars: mass-loss

Simbad objects: 32

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Number of rows : 32
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* V523 Cas SB* 00 40 06.2679105096 +50 14 15.518292216   11.698 10.62 9.969 9.388 K4V 174 0
2 V* V366 Cas EB* 01 08 25.5892998144 +58 44 16.757142468   12.496 12.00 11.678 11.292 G1: 36 0
3 V* AD Phe SB* 01 16 38.0703906768 -39 42 31.330964628   11.06 10.47     F9/G0V 55 0
4 V* GW Cep EB* 01 45 58.6227384192 +80 04 55.327969128   11.72 11.21 11.025 10.656 G3 69 0
5 V* VY Cet EB* 01 49 33.6929873856 -19 37 29.231904252   12.09 11.48 11.006 10.323 ~ 38 0
6 V* UZ Oct EB* 04 43 35.9677526712 -84 48 39.999528900   9.72 9.21     ~ 43 0
7 V* RS Col SB* 05 15 31.2443106552 -28 45 02.128147740   10.27 9.67     ~ 52 0
8 V* UV Lyn SB* 09 03 24.1259135160 +38 05 54.597192072   10.23 9.56 9.052 8.738 G3V 119 0
9 V* EZ Hya SB* 09 26 41.0604555912 -13 45 06.403376232   11.39 10.56 10.022 9.842 G2 68 0
10 V* XZ Leo SB* 10 02 34.1959390656 +17 02 47.140374840   10.79 10.37 10.385 10.173 A8/F0V 108 0
11 V* UZ Leo SB* 10 40 33.1849763352 +13 34 00.854970636   10.13 9.75 9.357 9.14 A9/F1V 146 0
12 V* AW UMa SB* 11 30 04.3160006304 +29 57 52.674404544   7.27   6.7   F0 302 0
13 V* CE Leo EB* 11 44 24.2554757472 +23 21 22.849119288   12.602 12.39 11.27 10.798 K 93 0
14 V* W Crv SB* 12 07 34.3580942256 -13 08 59.009877636   11.95 11.28 10.67 10.214 ~ 76 0
15 V* CC Com SB* 12 12 06.0378799056 +22 31 58.682832024   13.09 11.42 10.543 10.085 K4/5V 228 0
16 V* BI CVn SB* 13 03 16.4093237568 +36 37 00.640627644   10.99 10.31 9.908 9.593 F9V 102 0
17 V* AW Vir EB* 13 27 32.8814859576 +03 02 28.513564980   11.85 11.30 10.516 10.157 F8 57 0
18 V* RR Cen SB* 14 16 57.2208600552 -57 51 15.656888844 7.70 7.65 7.29     A9/F0V 160 0
19 V* VW Boo SB* 14 17 26.0324550672 +12 34 03.446878260   11.33 10.55 10.054 9.777 G5V 117 0
20 V* AU Ser SB* 15 56 49.4686990368 +22 16 01.590650328   11.76 11.04 10.383 9.931 G4V 111 0
21 V* BF Pav EB* 18 45 39.3192203448 -59 38 25.869586416   12.80 12.20     ~ 24 0
22 * eps CrA SB* 18 58 43.3827144528 -37 06 26.380732536   5.24 4.85     F4VFe-0.8+ 224 0
23 V* V803 Aql EB* 19 00 44.1859567344 -07 28 53.971847148           ~ 35 0
24 V* OO Aql SB* 19 48 12.6525764880 +09 18 32.374957356   10.26 9.49 8.773 8.762 F9V 239 0
25 V* LT Pav EB* 19 48 36.1003313880 -71 01 33.734700804           F9-G0 17 0
26 V* V700 Cyg SB* 20 31 05.2474963704 +38 47 00.460821408   12.36 11.14 11.468 11.045 G2V 78 0
27 V* VW Cep SB* 20 37 21.6316723003 +75 36 01.894463230   8.13   7.0   G8V+K0V 561 0
28 V* MW Pav SB* 20 46 27.7481505168 -71 56 58.466402412   9.15 8.79     F3IV/V 83 0
29 V* RW PsA EB* 22 09 46.9301030376 -27 04 01.524226476   11.93 11.16     ~ 40 0
30 V* BB Peg SB* 22 22 56.8915406208 +16 19 27.861694716   11.69 11.17     F8V 124 0
31 V* EM Lac EB* 22 23 54.7818645024 +54 01 09.271578684   13.088 12.50 12.105 11.7 ~ 44 0
32 V* VZ Psc EB* 23 27 48.3881626645 +04 51 23.937175287   11.347 10.274 10.090 8.926 K4/5V 125 0

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