2010MNRAS.403.1633P


Query : 2010MNRAS.403.1633P

2010MNRAS.403.1633P - Mon. Not. R. Astron. Soc., 403, 1633-1656 (2010/April-3)

3D models of radiatively driven colliding winds in massive O + O star binaries - II. Thermal radio to submillimetre emission.

PITTARD J.M.

Abstract (from CDS):

In this paper, the thermal emission over cm to submillimetre (submm) wavelengths from the winds in short-period O + O star binaries is investigated (potential non-thermal emission is presently ignored). The calculations are based on 3D hydrodynamical models which incorporate gravity, the driving of the winds, orbital motion of the stars and radiative cooling of the shocked plasma. The thermal emission arises from the stellar winds and the region where they collide. We investigate the flux and spectrum from a variety of models as a function of orbital phase and orientation of the observer, and compare to the single star case. The emission from the wind-wind collision region (WCR) is strongly dependent on its density and temperature, being optically thick in radiative systems and optically thin in adiabatic systems. The flux from systems where the WCR is highly radiative, as investigated for the first time in this paper, can be over an order of magnitude greater than the combined flux from identically typed single stars. This excess occurs over a broad range of wavelengths from cm to submm. In contrast, when the WCR is largely adiabatic, a significant excess in the thermal flux occurs only below 100GHz.

In circular systems with (near) identical stars, the observed variability in synthetic light curves is typically less than a factor of 2. Eccentric systems may show order of magnitude or greater flux variability, especially if the plasma in the WCR transitions from an adiabatic to a radiative state and vice-versa - in such cases, the flux can display significant hysteresis with stellar separation. We further demonstrate that clumping can affect the variability of radio light curves.

We investigate the spectral index of the emission, and often find indices steeper than +0.6. Synthetic images display a variety of morphologies, with the emission sometimes resembling an intertwined `double-helix'. We conclude by comparing our results to observations. The predictions made in this paper are of interest to future observations with the next generation of radio and submm telescopes, including the EVLA, e-MERLIN, ALMA and the Square Kilometre Array, and future upgrades to the VLBA.


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

Journal keyword(s): shock waves - binaries: general - stars: early-type - stars: mass loss - stars: winds, outflows - radio continuum: stars

Simbad objects: 35

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Number of rows : 35
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 * iot Ori SB* 05 35 25.9861932063 -05 54 35.598684624 1.45 2.53 2.77     O9IIIvar 793 0
2 HD 47129 SB* 06 37 24.0420854544 +06 08 07.369104444 5.23 6.11 6.06     O8I+O7.5III 420 0
3 * gam02 Vel WR* 08 09 31.95013 -47 20 11.7108 0.64 1.58 1.83 1.85 2.00 WC8+O7.5III-V 951 0
4 HD 93129 ** 10 43 57.462360 -59 32 51.27000 6.26 7.840 7.884 7.839   O2If*+O3.5V((f)) 208 1
5 HD 93161A SB* 10 44 08.8380609288 -59 34 34.509718560 7.33 8.619 8.581 8.61   O7.5V+O9V 52 1
6 V* V560 Car SB* 10 44 33.7393258944 -59 44 15.434446956 6.89 7.80 7.75 7.56 7.46 O3.5V((f))+O8V 314 0
7 * eta Car s*b 10 45 03.545808 -59 41 03.95124 6.37 7.03 6.48 6.123 4.41 LBV 2543 0
8 HD 93403 SB* 10 45 44.1198371784 -59 24 28.153300860 6.72 8.46 8.27 8.35   O5.5III(fc)var 203 1
9 Cl Westerlund 1 OpC 16 47 02.4 -45 51 07           ~ 655 1
10 NAME Sco OB 1 As* 16 53.5 -41 57           ~ 222 0
11 HD 152248 Y*O 16 54 10.0618206816 -41 49 30.139291596 5.56 6.15 6.088     O7Iabf+O7Ib(f) 270 0
12 CD-38 11746 WR* 17 19 00.5232022104 -38 48 51.247595664 13.01 12.48 11.02 10.55   WN8h 106 0
13 HD 159176 Be* 17 34 42.4921337376 -32 34 53.995451196 4.88 5.74 5.70 7.19   O7V 261 0
14 WR 98a WR* 17 41 13.0411858104 -30 32 30.409373688   18.40   15.20 13.82 WC8/9 112 1
15 [FNG2002] 19 Rad 17 45 49.82 -28 49 26.5           ~ 11 0
16 WR 102ad WR* 17 45 50.22 -28 49 21.9           WN8-9 27 0
17 [YLW2002] A1S X 17 45 50.3 -28 49 22           ~ 7 0
18 WR 102ah WR* 17 45 50.43 -28 49 21.9           WN8-9h 33 0
19 WR 102ai WR* 17 45 50.47 -28 49 31.5           WN8-9 19 0
20 WR 102aj WR* 17 45 50.48 -28 49 19.2           WN8-9h 29 0
21 NAME Arches Cluster Cl* 17 45 50.5 -28 49 28           ~ 792 0
22 [YLW2002] A1N X 17 45 50.5 -28 49 19           ~ 7 0
23 NAME Quintuplet Cluster OpC 17 46 13.9 -28 49 48           ~ 561 0
24 WR 102d WR* 17 46 14.05 -28 49 16.5           WN9 21 0
25 [LFG99] QR6 Rad 17 46 15.14 -28 49 32.7           ~ 7 0
26 [LFG99] QR9 Rad 17 46 17.98 -28 49 03.4           ~ 3 0
27 MR 80 WR* 18 02 04.1244400656 -23 37 42.168277056   15.002 13.155 12.056   WC9 241 1
28 HD 165052 SB* 18 05 10.5506592816 -24 23 54.847798080 6.16 6.98 6.87 7.77   O6.5V((f))z 282 1
29 HD 167971 s*b 18 18 05.8947362832 -12 14 33.313601112 7.89 8.27 7.50 6.68 6.279 O8Iaf(n)+O4/5 324 0
30 HD 168112 SB* 18 18 40.8671461608 -12 06 23.367244644 8.81 9.21 8.52 9.24   O5III(f) 156 0
31 HD 168206 WR* 18 19 07.3629298440 -11 37 59.164994424 9.65 9.88 9.10     WC8+O8/9III/V 308 1
32 HD 193077 WR* 20 17 00.0260987184 +37 25 23.785483116 7.82 8.32 8.01 8.71   WN5o+B? 297 0
33 Schulte 9 s*b 20 33 10.7362926720 +41 15 08.222370372 13.38 12.77 10.96     O5I+O4III 243 0
34 BD+40 4227A SB* 20 33 15.0781182864 +41 18 50.479292556 10.42 10.27 8.98 8.03 6.83 O6Ib(fc)+O4.5:III:(fc) 253 0
35 HD 215835 SB* 22 46 54.1107754872 +58 05 03.533752788 8.24 8.85 8.629   8.049 O5.5V((f))+O6V((f)) 260 0

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