4.7 Article

Massive stars and the energy balance of the interstellar medium.: II.: The 35 M⊙ star and a solution to the missing wind problem

Journal

ASTROPHYSICAL JOURNAL
Volume 638, Issue 1, Pages 262-280

Publisher

UNIV CHICAGO PRESS
DOI: 10.1086/498734

Keywords

HII regions; hydrodynamics; ISM : bubbles; ISM : individual (S308); ISM : structure; X-rays : individual (S308)

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We continue our numerical analysis of the morphological and energetic influence of massive stars on their ambient interstellar medium for a 35 M-circle dot star that evolves from the main-sequence through red supergiant and Wolf-Rayet phases, until it ultimately explodes as a supernova. We find that structure formation in the circumstellar gas during the early main-sequence evolution occurs as in the 60 M-circle dot case but is much less pronounced because of the lower mechanical wind luminosity of the star. On the other hand, since the shell-like structure of the H-II region is largely preserved, effects that rely on this symmetry become more important. At the end of the stellar lifetime 1% of the energy released as Lyman continuum radiation and stellar wind has been transferred to the circumstellar gas. From this fraction 10% is kinetic energy of bulk motion, 36% is thermal energy, and the remaining 54% is ionization energy of hydrogen. The sweeping up of the slow red supergiant wind by the fast Wolf-Rayet wind produces remarkable morphological structures and emission signatures, which are compared with existing observations of the Wolf-Rayet bubble S308, whose central star has probably evolved in a manner very similar to our model star. Our model reproduces the correct order of magnitude of observed X-ray luminosity, the temperature of the emitting plasma, and the limb brightening of the intensity profile. This is remarkable, because current analytical and numerical models of Wolf-Rayet bubbles fail to consistently explain these features. A key result is that almost the entire X-ray emission in this stage comes from the shell of red supergiant wind swept up by the shocked Wolf-Rayet wind rather than from the shocked Wolf- Rayet wind itself as hitherto assumed and modeled. This offers a possible solution to what is called the missing wind problem of Wolf-Rayet bubbles.

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