2008
DOI: 10.1086/589760
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The Effects of Clumps in Explaining X‐Ray Emission Lines from Hot Stars

Abstract: It is now well established that stellar winds of hot stars are fragmentary and that the X-ray emission from stellar winds has a strong contribution from shocks in winds. Chandra high spectral resolution observations of line profiles of O and B stars have shown numerous properties that had not been expected. Here we suggest explanations by considering the X-rays as arising from bow shocks that occur where the stellar wind impacts on spherical clumps in the winds. We use an accurate and stable numerical hydrodyn… Show more

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Cited by 25 publications
(41 citation statements)
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“…Exceptionally large, pancake-shaped clumps which form close to the photosphere at low velocities would resist the radiative acceleration. Being an obstacle to the generally much faster wind, they create strong reverse shocks that may add more mass to the clump if the gas cools quickly, or generate bow shocks if it does not (Cassinelli et al 2008). Self-consistent kinematic models of Gayley (in prep.…”
Section: On the Origin Of X-ray Emission In Wr Starsmentioning
confidence: 99%
“…Exceptionally large, pancake-shaped clumps which form close to the photosphere at low velocities would resist the radiative acceleration. Being an obstacle to the generally much faster wind, they create strong reverse shocks that may add more mass to the clump if the gas cools quickly, or generate bow shocks if it does not (Cassinelli et al 2008). Self-consistent kinematic models of Gayley (in prep.…”
Section: On the Origin Of X-ray Emission In Wr Starsmentioning
confidence: 99%
“…By contrast the case of clump bow-shocks indicate that the spatial correlation of cool and hot components can in principle produce reasonable emission line profiles. However, the simulations of Cassinelli et al (2008) did not evolve a clump through the flow. Instead, Ignace et al (2012) made use of beta velocity laws to impose a velocity difference between the clumps and interclump gas.…”
Section: Discussionmentioning
confidence: 97%
“…Since these winds are clumped, this emission is likely to originate from bow shocks forming around clumps. The Cassinelli et al (2008) wind bow shock model predicts that the temperature dependence of the emission measure scales as (T /T max ) −4/3 , where T max is the temperature at the apex of the bow shock. Hence, there should be a considerable amount of XUV radiation, even for rather strong shocks, located at any radius.…”
Section: Discussionmentioning
confidence: 99%