A Two-temperature Statistical Model for Particle Production at High Energies
Two-temperature statistical model for particle production at high energies
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Two-temperature statistical model for particle production at high energies
Electrostatic energy per degree of freedom of two-temperature plasma examined for validity of resonant approximations in ion wave region
Two-temperature model for examining particle spectra from proton-proton and proton nuclei interactions at machine energies
Analysis of ionized plasmas in which electron temperature exceeds ion temperature
Particle momentum distributions derived from relativistic quantum statistical mechanics
FORTRAN program for calculating particle spectra produced in high energy proton-proton collisions by two temperature statistical model
Secondary particle spectra from proton-proton interactions analyzed in two temperature statistical model, considering momentum distributions
Radiative transfer, chemical nonequilibrium, and two temperature effects behind reflected shock wave in nitrogen
Flowfields behind reflected shock waves, predicting end-wall radiative heat transfer and radiative gas dynamic coupling effects
Long wavelength ion acoustic instability of two temperature collisional fully ionized plasma with heat transfer, noting additional destabilizing currents
From a perturbation analysis of the fluid equations for a homogeneous unmagnetized plasma, it is shown that long wavelength ion waves are unstable when the electron temperature exceeds the ion temperature. Thus, the temperature difference can drive a resistive-type ion wave instability in a plasma which on a collisionless basis is stable. The additional destabilizing effect of a current is also investigated.
Study of deviations from thermal equilibrium among the ions in the ionosphere by considering that the 'light' ions H(+) and He(+) may be at a different temperature from the 'heavy' ion O(+). In particular, the case in which thermal protons are observed to be flowing relative to the assumed static ambient oxygen ions is considered. The proton flow is assumed to be along the direction of the magnetic field. Of the cases tested, it is found that the measured proton temperature is from one to ten times the measured oxygen ion temperature. Such temperature enhancements may be expected both because of the energy transfer associated with the ion flow and as a consequence of the preferential energy coupling from the light-ion distribution in the exosphere.
HF conductivity of quasi-equilibrium isotropic fully ionized two-temperature plasma
Dielectric constant of homogeneous fully ionized two-temperature plasma for determining conditions under which ion waves can be found
Homogeneous, fully ionized plasma HF conductivity computed using kinetic equation, showing application to two-temperature plasma
Heat transfer analysis procedure is presented for two-temperature gaseous plasma. Analysis is based on laminar flow of singly-ionized, quasineutral plasma with variable properties. Sheath analysis is described for species in accelerating field, decelerating field, emitted from wall, and recombining at wall.
The electron temperatures that would be determined (using the conventional single-temperature analysis) by the electrostatic probe, the diffuse resonance, and the radar backscatter techniques in an isotropic two-temperature plasma are presented. Plasma models corresponding to the addition of a minor component of energetic electrons and models corresponding to a process that cools a fraction of the ionospheric electrons are considered. The diffuse resonance temperature is found to lie between the probe and radar backscatter temperatures. The isotropic models corresponding to the addition of energetic electrons cannot support the reported discrepancies between radio wave and probe electron temperature measurements. Temperature differences similar to the observed differences can be produced by models with a fraction of the electrons at a temperature cooler than that of the main component of electrons. These models, however, are difficult to explain in terms of present understanding of the ionospheric plasma.
The microscopic physics of the thermonuclear runaway in highly degenerate carbon-oxygen cores is investigated to determine if and how a detonation wave is generated. An expression for the electron-ion relaxation time is derived under the assumption of large degeneracy and extreme relativity of the electrons in a two-temperature plasma. Since the nuclear burning time proves to be several orders of magnitude shorter than the relaxation time, it is concluded that in studying the structure of the detonation wave the electrons and ions must be treated as separate fluids.