scholarly journals THREE-DIMENSIONAL RADIATION-HYDRODYNAMICS CALCULATIONS OF THE ENVELOPES OF YOUNG PLANETS EMBEDDED IN PROTOPLANETARY DISKS

2013 ◽  
Vol 778 (1) ◽  
pp. 77 ◽  
Author(s):  
Gennaro D'Angelo ◽  
Peter Bodenheimer
2007 ◽  
Vol 464 (2) ◽  
pp. 429-435 ◽  
Author(s):  
M. González ◽  
E. Audit ◽  
P. Huynh

2018 ◽  
Vol 857 (1) ◽  
pp. 57 ◽  
Author(s):  
Riouhei Nakatani ◽  
Takashi Hosokawa ◽  
Naoki Yoshida ◽  
Hideko Nomura ◽  
Rolf Kuiper

2018 ◽  
Vol 865 (1) ◽  
pp. 75 ◽  
Author(s):  
Riouhei Nakatani ◽  
Takashi Hosokawa ◽  
Naoki Yoshida ◽  
Hideko Nomura ◽  
Rolf Kuiper

2018 ◽  
Vol 14 (S343) ◽  
pp. 9-18
Author(s):  
Bernd Freytag ◽  
Susanne Höfner ◽  
Sofie Liljegren

AbstractLocal three-dimensional radiation-hydrodynamics simulations of patches of the surfaces of solar-type stars, that are governed by small-scale granular convection, have helped analyzing and interpreting observations for decades. These models contributed considerably to the understanding of the atmospheres and indirectly also of the interiors and the active layers above the surface of these stars. Of great help was of course the availability of a close-by prototype of these stars – the sun.In the case of an asymptotic-giant-branch (AGB) star, the convective cells have sizes comparable to the radius of the giant. Therefore, the extensions of the solar-type-star simulations to AGB stars have to be global and cover the entire object, including a large part of the convection zone, the molecule-formation layers in the inner atmosphere, and the dust-formation region in the outer atmosphere. Three-dimensional radiation-hydrodynamics simulations with CO5BOLD show how the interplay of large and small convection cells, waves, pulsations, and shocks, but also molecular and dust opacities of AGB stars create conditions very different from those in the solar atmosphere.Recent CO5BOLD models account for frequency-dependent radiation transport and the formation of two independent dust species for an oxygen-rich composition. The drop of the comparably smooth temperature distribution below a threshold determines to onset of dust formation, further in, at higher temperatures, for aluminium oxides (Al2O3) than for silicates (Mg2SiO4). An uneven dust distribution is mostly caused by inhomogeneities in the density of the shocked gas.


2008 ◽  
Vol 4 (S258) ◽  
pp. 383-394 ◽  
Author(s):  
Pierre Demarque

AbstractA brief summary of the history of stellar evolution theory and the use of isochrones is given. The present state of the subject is summarized. The major uncertainties in isochrone construction are considered: chemical abundances and color calibrations, and the treatment of turbulent convection in stellar interior and atmosphere models. The treatment of convection affects the modeling of stellar interiors principally in two ways: convective core overshoot which increases evolutionary lifetimes, and the depth of convection zones which determines theoretical radii. Turbulence also modifies atmospheric structure and dynamics, and the derivation of stellar abundances. The symbiosis of seismic techniques with increasingly more realistic three-dimensional radiation hydrodynamics simulations is transforming the study of late-type stars. The important case of very low mass stars, which are fully convective, is briefly visited.


2016 ◽  
Vol 827 (2) ◽  
pp. 144 ◽  
Author(s):  
M. Flock ◽  
S. Fromang ◽  
N. J. Turner ◽  
M. Benisty

2006 ◽  
Vol 18 ◽  
pp. 115-128
Author(s):  
E. Audit ◽  
M. González

2017 ◽  
Vol 16 (01) ◽  
pp. 85-102 ◽  
Author(s):  
Feng Xie ◽  
Christian Klingenberg

General radiation magnetic hydrodynamics models include two main parts that are coupled: one part is the macroscopic magnetic fluid part, which is governed by the ideal compressible magnetohydrodynamic (MHD) equations with additional radiation terms; another part is the radiation field, which is described by a transfer equation. It is well known that in radiation hydrodynamics without a magnetic field there are two physical approximations: one is the so-called P1 approximation and the other is the so-called gray approximation. Starting out with a general radiation MHD model one can derive the so-called MHD-P1 approximation model. In this paper, we study the non-relativistic type limit for this MHD-P1 approximation model since the speed of light is much larger than the speed of the macroscopic fluid. This way we achieve a rigorous derivation of a widely used macroscopic model in radiation magnetohydrodynamics.


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