2005AJ....129.1018H


Query : 2005AJ....129.1018H

2005AJ....129.1018H - Astron. J., 129, 1018-1034 (2005/February-0)

VLA observations of ζ Aurigae: confirmation of the slow acceleration wind density structure.

HARPER G.M., BROWN A., BENNETT P.D., BAADE R., WALDER R. and HUMMEL C.A.

Abstract (from CDS):

Studies of the winds from single K and early M evolved stars indicate that these flows typically reach a significant fraction of their terminal velocity within the first couple of stellar radii. The most detailed spatially resolved information of the extended atmospheres of these spectral types comes from the ζ Aur eclipsing binaries. However, the wind acceleration inferred for the evolved primaries in these systems appears significantly slower than for stars of similar spectral type. Since there are no successful theories for mass loss from K and early M evolved stars, it is important to place strong empirical constraints on potential models and determine whether this difference in acceleration is real or an artifact of the analyses. We have undertaken a radio continuum monitoring study of ζ Aurigae (K4 Ib + B5 V) using the Very Large Array to test the wind density model of Baade et al. that is based on Hubble Space Telescope (HST) Goddard High Resolution Spectrograph ultraviolet spectra. ζ Aur was monitored at centimeter wavelengths over a complete orbital cycle, and flux variations during the orbit are found to be of similar magnitude to variations at similar orbital phases in the adjacent orbit. During eclipse, the flux does not decrease, showing that the radio emission originates from a volume substantially larger than R3K~(150R☉)3 surrounding the B star. Using the one-dimensional density model of the K4 Ib primary's wind derived from HST spectral line profile modeling and electron temperature estimates from previous optical and new HST studies, we find that the predicted radio fluxes are consistent with those observed. Three-dimensional hydrodynamic simulations indicate that the accretion flow perturbations near the B star do not contribute significantly to the total radio flux from the system, consistent with the radio eclipse observations. Our radio observations confirm the slow wind acceleration for the evolved K4 Ib component. ζ Aur's velocity structure does not appear to be typical of single stars with similar spectral types. This highlights the need for more comprehensive multiwavelength studies for both single stars, which have been sadly neglected, and other ζ Aur systems to determine if its wind properties are typical.

Abstract Copyright: ∼

Journal keyword(s): Stars: Binaries: Eclipsing - Radio Continuum: General - Stars: Individual: Constellation Name: ζ Aurigae - Stars: Mass Loss - Stars: Supergiants - Techniques: Interferometric

CDS comments: Par. 5, calibrators are JVAS J0432+416 and JVAS J0423+418

Simbad objects: 21

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Number of rows : 21
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 HD 6833 * 01 09 52.2648344184 +54 44 20.278107384 8.81 7.91 6.74     K0IIIbFe-2 204 0
2 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2924 2
3 NVSS J042355+415003 BLL 04 23 56.00979158 +41 50 02.7129362   19   19.2   ~ 123 1
4 2C 396 QSO 04 32 36.50262174 +41 38 28.4497778     20.0     ~ 231 1
5 * alf Tau LP? 04 35 55.23907 +16 30 33.4885 4.32 2.40 0.86 -0.37 -1.31 K5+III 1298 2
6 V* TX Cam Mi* 05 00 51.1627935408 +56 10 54.041462220       14.02   M9-9.5 365 0
7 * zet Aur SB* 05 02 28.6834429313 +41 04 32.995159760 5.35 4.97 3.75 2.62 1.75 K5II+B7V 470 0
8 * pi. Pup LP* 07 17 08.5580780520 -37 05 50.904468727 5.57 4.32 2.70 1.46 0.55 K4III 116 0
9 V* AL Vel SB* 08 31 11.2833125832 -47 39 57.413103300   9.43 8.65     K0III+A3III/V 68 0
10 * lam Vel s*r 09 07 59.75787 -43 25 57.3273 5.67 3.86 2.21 0.97 0.03 K4Ib 230 0
11 * alf Boo RG* 14 15 39.67207 +19 10 56.6730 2.46 1.18 -0.05 -1.03 -1.68 K1.5IIIFe-0.5 2417 1
12 * alf Sco s*r 16 29 24.45970 -26 25 55.2094 4.08 2.75 0.91 -0.64 -1.87 M1.5Iab+B2Vn 786 0
13 * alf TrA * 16 48 39.89508 -69 01 39.7626   3.33 1.88     K2III_Ba1 251 0
14 V* VX Sgr s*r 18 08 04.0442790744 -22 13 26.600899044 11.72 9.41 6.52 3.90 2.11 M8.5Ia 622 0
15 HD 169689 SB* 18 25 38.7990783216 +08 01 55.225743564   6.545 5.665     G9II+B9V 111 0
16 * 31 Cyg SB* 20 13 37.9082370480 +46 44 28.761618048 5.50 5.08 3.80 2.83 2.07 K3Ib+B2IV-V 385 0
17 * omi02 Cyg SB* 20 15 28.3242122880 +47 42 51.213932496 6.54 5.50 3.98 2.78 1.86 K7Ib-II+B1V 347 0
18 * 22 Vul SB* 20 15 30.2386386720 +23 30 32.051069712   6.192 5.176     G3Ib-II 215 0
19 * 47 Cyg s*r 20 33 54.1880917512 +35 15 03.039046848   6.145 4.636     K6:Ib+B2.5: 112 1
20 V* VV Cep s*r 21 56 39.1414963149 +63 37 31.981636440 7.03 6.65 4.90 3.19 1.85 M2Ibep+B2?ep_sh 466 0
21 * alf Aqr * 22 05 47.0355458275 -00 19 11.463439527 4.65 3.90 2.94 2.27 1.76 G2Ib 451 0

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