For non-equilibrium atmospheric mono-atomic plasmas the isentropic exponent is 1.2 for a large range of ionization degrees. The asymptotic dependence of the non-equilibrium parameters on the electron density is included. The small freedom of deviations from equilibrium expresses that the plasma tends to remain close to its equilibriu
The remarkable anticorrelation between ion temperature and density often seen in the plasma sheet is...
Non-equilibrium is one of the important features of an atmospheric gas discharge plasma. It involves...
The total radiative loss in atmospheric argon plasmas is calculated allowing for deviations from loc...
For non-equilibrium atmospheric mono-atomic plasmas the isentropic exponent is 1.2 for a large range...
The isentropic exponent for gases is a physical quantity that can ease significantly the hydrodynami...
The wide range of applications of cold plasmas originates from their special characteristi...
The electron temperature T/sub e/ is obtained from five optically non-thin Ar I line-transitions. It...
To describe plasmas in non-local thermal equilibrium (non-LTE) four parameters need to be used, whic...
To describe plasmas in non-local thermal equilibrium (non-LTE) four parameters need to be used, whic...
This paper, the second in the series, deals with the study of the impact of different types of equil...
Finite temperature effects on the relativistic radial equilibrium of a non-neutral plasma are analyz...
Abstract—Nonequilibrium effects associated with spatial and temporal nonlocality between electron en...
In this paper, we begin a systematic study of Non-Local Thermal Equilibrium (NLTE) phenomena in near...
The remarkable anticorrelation between ion temperature and density often seen in the plasma sheet is...
Non-equilibrium is one of the important features of an atmospheric gas discharge plasma. It involves...
The total radiative loss in atmospheric argon plasmas is calculated allowing for deviations from loc...
For non-equilibrium atmospheric mono-atomic plasmas the isentropic exponent is 1.2 for a large range...
The isentropic exponent for gases is a physical quantity that can ease significantly the hydrodynami...
The wide range of applications of cold plasmas originates from their special characteristi...
The electron temperature T/sub e/ is obtained from five optically non-thin Ar I line-transitions. It...
To describe plasmas in non-local thermal equilibrium (non-LTE) four parameters need to be used, whic...
To describe plasmas in non-local thermal equilibrium (non-LTE) four parameters need to be used, whic...
This paper, the second in the series, deals with the study of the impact of different types of equil...
Finite temperature effects on the relativistic radial equilibrium of a non-neutral plasma are analyz...
Abstract—Nonequilibrium effects associated with spatial and temporal nonlocality between electron en...
In this paper, we begin a systematic study of Non-Local Thermal Equilibrium (NLTE) phenomena in near...
The remarkable anticorrelation between ion temperature and density often seen in the plasma sheet is...
Non-equilibrium is one of the important features of an atmospheric gas discharge plasma. It involves...
The total radiative loss in atmospheric argon plasmas is calculated allowing for deviations from loc...
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