2019
DOI: 10.1051/0004-6361/201935991
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Non-LTE radiation hydrodynamics in PLUTO

Abstract: Context. Modeling the dynamics of most astrophysical structures requires an adequate description of the radiation-matter interaction. Several numerical (magneto)hydrodynamics codes were upgraded with a radiation module to fulfill this request. However, those among them that use either the flux-limited diffusion (FLD) or the M1 radiation moment approaches are restricted to the local thermodynamic equilibrium (LTE). This assumption may be not valid in some astrophysical cases. Aims. We present an upgraded versio… Show more

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Cited by 7 publications
(7 citation statements)
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“…This must be considered when interpreting the UV excess (see e.g. Calvet & Gullbring 1998;Hartmann et al 2016;Colombo et al 2019). We also expect a pre-heating of the accretion flow as a result of the EUV absorption.…”
Section: Synspec Monochromatic Emergent Intensitymentioning
confidence: 94%
See 1 more Smart Citation
“…This must be considered when interpreting the UV excess (see e.g. Calvet & Gullbring 1998;Hartmann et al 2016;Colombo et al 2019). We also expect a pre-heating of the accretion flow as a result of the EUV absorption.…”
Section: Synspec Monochromatic Emergent Intensitymentioning
confidence: 94%
“…However, as previously mentioned, such a study is computationally very demanding and is well beyond the scope of the present paper. Simplified NLTE models, as proposed by Colombo et al (2019), therefore are an interesting starting point in this new direction.…”
Section: Synspec: a Spectrum Synthesisermentioning
confidence: 99%
“…We have tested the code's ability to reproduce shock waves in optically thick media, in which the dynamical evolution of matter and radiation fields is coupled. We have reproduced the 1D setup considered in Ensman (1994), which is generally used as a standard benchmark in Rad-HD codes (see, e.g., Hayes & Norman 2003;González et al 2007;Commerçon et al 2011;Kolb et al 2013;Colombo et al 2019). In this configuration, both matter and radiation fields are initially uniform in a domain given by the interval [0, 7 × 10 10 ] cm.…”
Section: Radiative Shocksmentioning
confidence: 99%
“…where ρ is the plasma mass density, is the fluid velocity, k R and k P are, respectively, the Rosseland and Planck mean opacities, c the speed of light, F the comoving-frame radiation flux, E the plasma internal energy density, E the comoving-frame radiation energy, k B the Boltzmann constant, T the plasma temperature, µ the mean particle weight (assuming solar abundances), m H the hydrogen mass, λ the flux-limiter (Minerbo 1978), and γ = 5/3 the ratio of specific heats. In a companion paper (Colombo et al 2019a; in the following Paper I), we discuss the assumptions and the limits of these equations. Since we are interested in evaluating the effects of irradiation from the post-shock accreting material on the pre-shock accretion column, we neglect the radiation effects (both radiative losses and absorption of radiation by matter) in the pre-shock chromosphere (i.e., k P = k R = 0 and L = 0 in Eqs.…”
Section: The Radiation Hydrodynamics Modelmentioning
confidence: 99%