Thermal and gravitational instability of a model hydrogen plasma in the presence of a radiation field

1982 ◽  
Vol 68 (1) ◽  
pp. 39-48
Author(s):  
J. Manfroid ◽  
P. Grosjean
1967 ◽  
Vol 22 (12) ◽  
pp. 1953-1959 ◽  
Author(s):  
W.L. Bohn

Steady-state population densities and electron densities are calculated in a non-equilibrium hydrogen plasma at constant pressure. The ratio of the temperatures of electrons and heavy particles is taken as a parameter. The radiation field of the LYMAN lines is included using a mean absorption coefficient for each transition. The deviations of densities of excited levels and electrons from equilibrium values are very large at low temperatures. The ground state population remains closer to equilibrium until the resonance radiation field vanishes with increasing temperature. Deviations from equilibrium are found to be present even at atmospheric pressure. Detailed results are shown in numerous diagrams for pressures from 0.01 to 1 atmosphere and electron temperatures from 5 × 103 to 4×104°K.


2020 ◽  
Vol 640 ◽  
pp. A53
Author(s):  
L. Löhnert ◽  
S. Krätschmer ◽  
A. G. Peeters

Here, we address the turbulent dynamics of the gravitational instability in accretion disks, retaining both radiative cooling and irradiation. Due to radiative cooling, the disk is unstable for all values of the Toomre parameter, and an accurate estimate of the maximum growth rate is derived analytically. A detailed study of the turbulent spectra shows a rapid decay with an azimuthal wave number stronger than ky−3, whereas the spectrum is more broad in the radial direction and shows a scaling in the range kx−3 to kx−2. The radial component of the radial velocity profile consists of a superposition of shocks of different heights, and is similar to that found in Burgers’ turbulence. Assuming saturation occurs through nonlinear wave steepening leading to shock formation, we developed a mixing-length model in which the typical length scale is related to the average radial distance between shocks. Furthermore, since the numerical simulations show that linear drive is necessary in order to sustain turbulence, we used the growth rate of the most unstable mode to estimate the typical timescale. The mixing-length model that was obtained agrees well with numerical simulations. The model gives an analytic expression for the turbulent viscosity as a function of the Toomre parameter and cooling time. It predicts that relevant values of α = 10−3 can be obtained in disks that have a Toomre parameter as high as Q ≈ 10.


1991 ◽  
Vol 111 (7) ◽  
pp. 684-685
Author(s):  
Takao Kutsukake ◽  
Yoshimichi Ohki
Keyword(s):  

2003 ◽  
Vol 762 ◽  
Author(s):  
C. Smit ◽  
D.L. Williamson ◽  
M.C.M. van de Sanden ◽  
R.A.C.M.M. van Swaaij

AbstractExpanding thermal plasma CVD (ETP CVD) has been used to deposit thin microcrystalline silicon films. In this study we varied the position at which the silane is injected in the expanding hydrogen plasma: relatively far from the substrate and close to the plasma source, giving a long interaction time of the plasma with the silane, and close to the substrate, resulting in a short interaction time. The material structure is studied extensively. The crystalline fractions as obtained from Raman spectroscopy as well as from X-ray diffraction (XRD) vary from 0 to 67%. The average particle sizes vary from 6 to 17 nm as estimated from the (111) XRD peak using the Scherrer formula. Small angle X-ray scattering (SAXS) and flotation density measurements indicate void volume fractions of about 4 to 6%. When the samples are tilted the SAXS signal is lower than for the untilted case, indicating elongated objects parallel to the growth direction in the films. We show that the material properties are influenced by the position of silane injection in the reactor, indicating a change in the plasma chemistry.


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