Abstract:We have developed explicit quantum-mechanical expressions for the conductivity and resistivity tensors of a Lorentz plasma in a magnetic field. The expressions are based on a solution to the Boltzmann equation that is exact when the electric field is weak, the electron-Fermi-degeneracy parameter Theta>>1, and the electron-ion Coulomb-coupling parameter Gamma/Z<<1. (Gamma is the ion-ion coupling parameter and Z is the ion charge state.) Assuming a screened 1/r electron-ion scattering potential, we calculate the… Show more
“…Its advantages and drawbacks as well as the comparison with www.cpp-journal.org other theories have been discussed previously in many papers [1,2,18,19,38,39], where necessary details and derivation of the formulas are presented. So here we remark only that τ -approximation is correct in the same area where the developed chemical model is correct (see the last paragraph of previous section).…”
The pressure, internal energy, conductivity, thermal conductivity and thermal power of Iron plasma have been calculated at temperatures 10 -100 kK and densities less than 2 g/cm 3 . The plasma composition has been obtained by means of corresponding system of coupled mass action laws. We have considered the atom ionization up to +6. The transport coefficients have been obtained within the relaxation time approximation. The comparison of our results with available measurement and calculation data has shown very good agreement for the pressure and less good agreement for the conductivity.
“…Its advantages and drawbacks as well as the comparison with www.cpp-journal.org other theories have been discussed previously in many papers [1,2,18,19,38,39], where necessary details and derivation of the formulas are presented. So here we remark only that τ -approximation is correct in the same area where the developed chemical model is correct (see the last paragraph of previous section).…”
The pressure, internal energy, conductivity, thermal conductivity and thermal power of Iron plasma have been calculated at temperatures 10 -100 kK and densities less than 2 g/cm 3 . The plasma composition has been obtained by means of corresponding system of coupled mass action laws. We have considered the atom ionization up to +6. The transport coefficients have been obtained within the relaxation time approximation. The comparison of our results with available measurement and calculation data has shown very good agreement for the pressure and less good agreement for the conductivity.
“…This behavior is a result of the density-dependence of the nonideality corrections to the chemical potentials in eq. (12). COMPTRA04 treats the related instability as shown in Fig.…”
Section: In-and Output Files For the Calculation Of The Plasma Composmentioning
COMPTRA04 is a Fortran 90 program package developed for the calculation of composition and transport coefficients within the partially ionized plasma model. This paper summarizes the theoretical background and gives instructions on how to implement and use the package. Results obtained by using COMPTRA04 are given for Be plasma in order to allow for a test of the package.
“…For highly and moderately degenerate plasmas the influence of electron-electron collisions will be decreased due to Pauli blocking [52]. This effect can be taken into account, if one uses the expression for Spitzer factor in a degenerate electron plasma [53,54]:…”
A simple model for the dielectric function of a completely ionized plasma with an arbitrary ionic charge, that is valid for long-wavelength high-frequency perturbations is derived using an approximate solution of a linearized Fokker-Planck kinetic equation for electrons with a Landau collision integral. The model accounts for both the electron-ion collisions and the collisions of the subthermal (cold) electrons with thermal ones. The relative contribution of the latter collisions to the dielectric function is treated phenomenologically, introducing some parameter κ that is chosen in such a way as to get a well-known expression for stationary electric conductivity in the low-frequency region and fulfill the requirement of a vanishing contribution of electron-electron collisions in the high-frequency region. This procedure ensures the applicability of our model in a wide range of plasma parameters as well as the frequency of the electromagnetic radiation. Unlike the interpolation formula proposed earlier by Brantov et al. [Brantov et al., JETP 106, 983 (2008)
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