2015ApJ...812...40G


Query : 2015ApJ...812...40G

2015ApJ...812...40G - Astrophys. J., 812, 40 (2015/October-2)

Adiabatic mass loss in binary stars. II. From zero-age main sequence to the base of the giant branch.

GE H., WEBBINK R.F., CHEN X. and HAN Z.

Abstract (from CDS):

In the limit of extremely rapid mass transfer, the response of a donor star in an interacting binary becomes asymptotically one of adiabatic expansion. We survey here adiabatic mass loss from Population I stars (Z = 0.02) of mass 0.10 M☉-100 M☉ from the zero-age main sequence to the base of the giant branch, or to central hydrogen exhaustion for lower main sequence stars. The logarithmic derivatives of radius with respect to mass along adiabatic mass-loss sequences translate into critical mass ratios for runaway (dynamical timescale) mass transfer, evaluated here under the assumption of conservative mass transfer. For intermediate- and high-mass stars, dynamical mass transfer is preceded by an extended phase of thermal timescale mass transfer as the star is stripped of most of its envelope mass. The critical mass ratio qad(throughout this paper, we follow the convention of defining the binary mass ratio as q ≡ Mdonor/Maccretor) above which this delayed dynamical instability occurs increases with advancing evolutionary age of the donor star, by ever-increasing factors for more massive donors. Most intermediate- or high-mass binaries with nondegenerate accretors probably evolve into contact before manifesting this instability. As they approach the base of the giant branch, however, and begin developing a convective envelope, qad plummets dramatically among intermediate-mass stars, to values of order unity, and a prompt dynamical instability occurs. Among low-mass stars, the prompt instability prevails throughout main sequence evolution, with qaddeclining with decreasing mass, and asymptotically approaching qad= 2/3, appropriate to a classical isentropic n = 3/2 polytrope. Our calculated qadvalues agree well with the behavior of time-dependent models by Chen & Han of intermediate-mass stars initiating mass transfer in the Hertzsprung gap. Application of our results to cataclysmic variables, as systems that must be stable against rapid mass transfer, nicely circumscribes the range in qad as a function of the orbital period in which they are found. These results are intended to advance the verisimilitude of population synthesis models of close binary evolution.

Abstract Copyright: ∼

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

VizieR on-line data: <Available at CDS (J/ApJ/812/40): table1.dat table2.dat table3.dat>

Simbad objects: 38

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Number of rows : 38
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* HT Cas CV* 01 10 13.1213394144 +60 04 35.489642700     14.10     M5.5e 401 0
2 V* RW Tri CV* 02 25 36.1556820000 +28 05 50.891220600   13.50 12.50     M0V 324 0
3 V* VW Hyi CV* 04 09 11.3967378648 -71 17 41.554528260   12.786 12.543 14.160   DQ 661 0
4 V* XZ Eri CV* 04 11 25.7623081800 -15 23 23.764734528           ~ 60 0
5 V* V363 Aur CV* 05 33 33.4591265880 +36 59 32.475580692     14.2     K0V 107 0
6 V* V347 Pup CV* 06 10 33.6583947384 -48 44 25.363374036   13.95 13.57 13.24 12.79 M0.5V 103 0
7 V* BT Mon No* 06 43 47.2416090432 -02 01 13.876883184   15.737 14.638 15.411   G8V 183 0
8 V* U Gem CV* 07 55 05.2324414746 +22 00 05.044127985   15.3 14.54     DA 1135 0
9 V* Z Cha CV* 08 07 27.7517751528 -76 32 00.665029356           M5.5 620 1
10 V* AC Cnc CV* 08 44 27.1121665272 +12 52 31.995783264   13.80 14.15     K1-3V 154 0
11 CRTS J090350.7+330036 CV* 09 03 50.7253230816 +33 00 36.113249628           DQ: 32 0
12 V* GY Cnc CV* 09 09 50.5407550968 +18 49 47.429496300           ~ 87 0
13 V* DV UMa CV* 09 46 36.5964360384 +44 46 44.683031784   19.0       DA:+M 131 0
14 V* OY Car CV* 10 06 22.0793274312 -70 14 04.584660540           ~ 586 0
15 CRTS J100658.4+233724 CV* 10 06 58.4169543888 +23 37 24.466842948           D+M3e 35 0
16 V* DW UMa CV* 10 33 52.8751411128 +58 46 54.717259044   14.33   14.33 14.35 ~ 254 0
17 SDSS J103533.02+055158.4 CV* 10 35 33.0226966464 +05 51 58.334599512   18.57 18.80     DA 64 0
18 V* IY UMa CV* 10 43 56.7487980888 +58 07 31.920814488   17.52 16.61 17.62 17.60 ~ 119 0
19 SDSS J115207.00+404947.6 CV* 11 52 07.0049089008 +40 49 47.903371500           ~ 25 0
20 V* GP CVn CV* 12 27 40.8198845784 +51 39 24.962023620   18.89 19.08     DA+M 40 0
21 V* EX Hya CV* 12 52 24.2222471899 -29 14 55.999766523   13.505 13.491 13.549   M5-6V 730 0
22 V* V1258 Cen CV* 13 00 29.0630127912 -30 52 56.960840244           ~ 25 0
23 PM J14332+1011 CV* 14 33 17.7877088088 +10 11 23.484691356     18.86     ~ 60 0
24 V* OU Vir CV* 14 35 00.2216793576 -00 46 06.269754864   18.5       M2: 56 0
25 SDSS J150137.22+550123.4 CV* 15 01 37.2173710728 +55 01 23.280739320   18.2   18.8   DA: 35 0
26 V* NZ Boo CV* 15 02 41.0007781680 +33 34 24.002686380           ~ 47 0
27 V* OV Boo CV* 15 07 22.3698571080 +52 30 39.804859764   18.7   18.5   DAe 82 0
28 V* U Sco CV* 16 22 30.7791646104 -17 52 43.166822628           F8+K2 592 0
29 V* V1239 Her CV* 17 02 13.2462561912 +32 29 54.159948960           M1.5e 60 0
30 V* EX Dra No* 18 04 14.2485669582 +67 54 12.273781393   14.775 14.479 14.490   ~ 135 0
31 V* DQ Her CV* 18 07 30.2510391864 +45 51 32.564791872   14.605 14.443 14.800   M3+Ve 1048 1
32 V* AM Her CV* 18 16 13.2546725104 +49 52 04.759613537   15.124 14.808 13.525   M4.5-5Ve 1009 2
33 V* BD Pav CV* 18 43 11.9137504416 -57 30 44.865618300           ?+K 72 0
34 V* EM Cyg CV* 19 38 40.1068970904 +30 30 28.332591012     11.90     ~ 270 0
35 V* WZ Sge CV* 20 07 36.5037622512 +17 42 14.733254952   15.30 15.20 10.817   D 982 0
36 V* AE Aqr CV* 20 40 09.1598959176 -00 52 15.055595220   12.46 10.40   10.191 K3-5IV/V 705 0
37 V* IP Peg CV* 23 23 08.5362249504 +18 24 59.206884012           M2 395 0
38 V* DI Phe CV* 23 54 20.4574289520 -47 00 20.249299224           ~ 12 0

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