Interaction of High-Pressure Arc Plasmas with Thermionic Cathodes

On-Line Tool for Simulation of Different Modes of Axially Symmetric Current Transfer to Cathodes of High-Pressure Arc Discharges
 

What is this code destined for?
The objective of this code is two-fold. The first one is to provide a fast and robust tool for simulation of diffuse and axially symmetric spot modes of current transfer from high-pressure plasmas to cylindrical thermionic cathodes in a wide range of arc currents, cathode materials and dimensions, and plasma compositions. The second objective is methodical. Nowadays, it is universally understood that different modes of current transfer to thermionic cathodes are described by multiple solutions that must exist under certain discharge conditions in an adequate theoretical model. Unfortunately, the concept of multiple solutions, while being quite common in many areas of theoretical physics, is not equally widespread in applied physics. Therefore, we tried to offer to applied physicists and engineers working in the field a tutorial that would help them to make themselves comfortable with multiple solutions describing different modes of current transfer to thermionic cathodes. Is should be stressed that the experience gained with this tutorial will facilitate work with other solvers, including commercial software like COMSOL Multiphysics or ANSYS: difficulties encountered in finding multiple solutions by means of any efficient solver are the same.

The code is based on the model of nonlinear surface heating [see, e.g., review M. S. Benilov, Understanding and modelling plasma–electrode interaction in high-pressure arc discharges: a review, J. Phys. D: Appl. Phys. 41, No. 14, pp. 144001-1-30 (2008) and references therein] and consists of three modules. The first module provides a solution describing the near-cathode plasma layer. The second module provides a solution of the heat conduction equation in the cathode body under the assumption of axial symmetry. The third module is dedicated to calculation of bifurcation points positioned on the axially symmetric modes, in particular, of the limit of stability of the diffuse mode.

The code is written in Fortran and is quite fast and robust. The database includes a large variety of plasma-producing gases (in particular, He, Ne, Na, Ar, Cu, Kr, Xe, Cs, Hg, air, mixture Na-Hg, mixture Cs-Hg, plasmas of mercury with addition of metal halides, plasmas of xenon with addition of metal halides) and of cathode materials (in particular, W, Mo, Fe, Nb, and Zr).
Current-voltage characteristics of different steady-state modes and typical distributions of the temperature of the cathode surface associated with each mode. Circles: bifurcation points. W cathode, R = 2mm, h = 10mm, Tc = 300K, Ar plasma, p = 1bar.

An example of current-voltage characteristics (CVCs) of different steady-state modes is shown in the figure. For U exceeding approximately 14V, nine different steady state are possible. Five of these states (those with spots at the edge of the front surface of the cathode) are 3D. The code is destined for finding the four states are axially symmetric:

and also for finding bifurcation points at which 3D modes branch off from the axially symmetric modes (note that one of these points represents the limit of stability of the diffuse mode).

To whom is this code destined?
The code is destined to researchers and engineers working on high-pressure arc discharges. It can be used

Conditions of use
The code is free for non-commercial personal use only. Simulation results must not be transferred to third parties, however they may be used for producing scientific publications, provided that the references are made to the paper M. S. Benilov, M. D. Cunha, and G. V. Naidis, Modelling interaction of multispecies plasmas with thermionic cathodes, Plasma Sources Sci. Technol. 14, No. 3, pp. 517-524 (2005) and to this site (http://www.arc_cathode.uma.pt).

Disclaimer
The code is made available "AS IS" without warranty of any kind. The entire risk as to the results and the performance of the code is assumed by the user, and in no event will the authors be liable for any consequential, incidental or direct damages suffered in the course of using the code.

 
 
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