Issue |
A&A
Volume 665, September 2022
|
|
---|---|---|
Article Number | A35 | |
Number of page(s) | 18 | |
Section | Interstellar and circumstellar matter | |
DOI | https://doi.org/10.1051/0004-6361/202243531 | |
Published online | 09 September 2022 |
Thermal emission from bow shocks
II. 3D magnetohydrodynamic models of ζ Ophiuchi
1
Dublin Institute for Advanced Studies, Astronomy & Astrophysics Section,
31 Fitzwilliam Place,
Dublin 2, Ireland
e-mail: green@cp.dias.ie
2
Centre for AstroParticle Physics and Astrophysics, DIAS Dunsink Observatory,
Dunsink Lane,
Dublin 15, Ireland
3
School of Physics, University College Dublin,
Belfield,
Dublin 4, Ireland
4
Astronomy Unit, School of Physics and Astronomy, Queen Mary University of London,
London
E1 4NS, UK
5
Sternberg Astronomical Institute, Lomonosov Moscow State University,
Universitetskij Pr. 13,
Moscow
119992, Russia
6
Space Research Institute, Russian Academy of Sciences,
Profsoyuznaya 84/32,
117997
Moscow, Russia
Received:
12
March
2022
Accepted:
26
May
2022
The nearby, massive, runaway star ζ Ophiuchi has a large bow shock detected in optical and infrared light and, uniquely among runaway O stars, diffuse X-ray emission detected from the shocked stellar wind. Here we make the first detailed computational investigation of the bow shock of ζ Ophiuchi, to test whether a simple model of the bow shock can explain the observed nebula, and to compare the detected X-ray emission with simulated emission maps. We reanalysed archival Chandra observations of the thermal diffuse X-ray emission from the shocked wind region of the bow shock, finding total unabsorbed X-ray flux in the 0.3–2keV band corresponding to a diffuse X-ray luminosity of LX = 2.33−1.54+1.12 × 1029 erg s−1, consistent with previous work. The diffuse X-ray emission arises from the region between the star and the bow shock. Three-dimensional magnetohydrodyanmic simulations were used to model the interaction of the star’s wind with a uniform interstellar medium (ISM) using a range of stellar and ISM parameters motivated by observational constraints. Synthetic infrared, Hα, soft X-ray, emission measure, and radio 6 GHz emission maps were generated from three simulations, for comparison with the relevant observations. Simulations where the space velocity of ζ Ophiuchi has a significant radial velocity produce infrared emission maps with the opening angle of the bow shock in better agreement with observations than for the case where motion is fully in the plane of the sky. All three simulations presented here have X-ray emission fainter than observed, in contrast to results for NGC 7635. The simulation with the highest pressure has the closest match to X-ray observations, with a flux level within a factor of two of the observational lower limit, and emission weighted temperature of log10(TA/K) = 6.4, although the morphology of the diffuse emission appears somewhat different. The observed X-ray emission is from a filled bubble that is brightest near the star, whereas simulations predict brightening towards the contact discontinuity as density increases. This first numerical study of the bow shock and wind bubble around ζ Ophiuchi uses a relatively simple model of a uniform ISM and ideal-magnetohydrodynamics, and can be used as a basis for comparing results from models incorporating more physical processes, or higher resolution simulations that may show more turbulent mixing.
Key words: hydrodynamics / instabilities / radiative transfer / methods: numerical / stars: winds, outflows / ISM: bubbles
© S. Green et al. 2022
Open Access article, published by EDP Sciences, under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
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