Investigation of the short argon arc with hot anode. II. Analytical model (original) (raw)

A short atmospheric pressure argon arc is studied numerically and analytically. In a short arc with an inter-electrode gap of several millimeters, non-equilibrium effects in plasma play an important role in operation of the arc. High anode temperature leads to electron emission and intensive radiation from its surface. A complete, self-consistent analytical model of the whole arc comprising of models for near-electrode regions, arc column, and a model of heat transfer in cylindrical electrodes was developed. The model predicts the width of non-equilibrium layers and arc column, voltages and plasma profiles in these regions, and heat and ion fluxes to the electrodes. Parametric studies of the arc have been performed for a range of the arc current densities, inter-electrode gap widths, and gas pressures. The model was validated against experimental data and verified by comparison with numerical solution. Good agreement between the analytical model and simulations and reasonable agreement with experimental data were obtained.

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Computing anode heating voltage in high-pressure arc discharges and modelling rod electrodes in dc and ac regimes

Journal of Physics D: Applied Physics, 2017

Numerical modelling of near-anode layers in arc discharges in several gases (Ar, Xe, and Hg) is performed in a wide range of current densities, anode surface temperatures, and plasma pressures. It is shown that the density of energy ‡ux to the anode is only weakly a¤ected by the anode surface temperature and varies linearly with the current density. This allows one to interpret the results in terms of anode heating voltage (volt equivalent of the heat ‡ux to the anode). The computed data may be useful in di¤erent ways. An example considered in this work concerns the evaluation of thermal regime of anodes in the shape of a thin rod operating in the di¤use mode. Invoking the model of nonlinear surface heating for cathodes, one obtains a simple and free of empirical parameters model of thin rod electrodes applicable to dc and ac high-pressure arcs provided that no anode spots are present. The model is applied to a variety of experiments reported in the literature and a good agreement with the experimental data found.

Novel non-equilibrium modelling of a DC electric arc in argon

Journal of Physics D: Applied Physics

View the article online for updates and enhancements. Related content Account of near-cathode sheath in numerical models of high-pressure arc discharges M S Benilov, N A Almeida, M Baeva et al.-Comparing two non-equilibrium approaches to modelling of a free-burning arc M Baeva, D Uhrlandt, M S Benilov et al.-Understanding and modelling plasma-electrode interaction in highpressure arc discharges M S Benilov-Recent citations Gas tungsten arc models including the physics of the cathode layer: remaining issues Isabelle Choquet-Main Issues for a Fully Predictive Plasma Spray Torch Model and Numerical Considerations Christophe Chazelas et al-Numerical Simulation of Nonequilibrium Species Diffusion in a Low-Power Nitrogen-Hydrogen Arcjet Thruster Hai-Xing Wang et al

Cold-electrode voltage fall for impulse arcs in argon between copper electrodes

Journal of Physics: Conference Series, 2011

The full electric arc discharge in gases for short gaps in homogeneous electric field and pressure·distance (pd) below 150 Torr·cm, can be described as a transition between different discharge mechanisms such as: Townsend, glow, and arc. Once the arc is achieved the measured voltage drops to some volts and the current density increases several orders of magnitude. Depending upon the type of gas used, the electrode surface characteristics and type of electrical excitation, the cathode and anode voltage fall might change. The present work is directed to study the electrode fall (sum of anode and cathode falls) during a current impulse arc discharge between copper electrodes in ceramic tubes filled with argon between 0.01 and 6.5 Torr·cm. The copper electrodes were cleaned, degassed and hydrogen reduced. The arc voltages were measured with fast/slow rise times and short/long duration current impulses produced by a RLC circuit. An increasing variation of the electrode fall was found at the pressure·distance range analyzed.

Effect of a bidirectional coupling of an LTE arc column to a refractory cathode in atmospheric pressure argon

Physics of Plasmas, 2020

An appropriate coupling of an arc plasma column in the state of local thermodynamic equilibrium to a refractory cathode necessarily involves the non-equilibrium boundary layer between them. A model has been developed that combines a model of an equilibrium direct current arc plasma in atmospheric pressure argon with the assembly of a cathode made of tungsten and the boundary layer. A bidirectional coupling has been realized that allows us to consider a variable voltage drop across the boundary layer for different positions on the cathode. The results are obtained for arc currents between 10 and 150 A in the cases of both a unidirectional and a bidirectional coupling. The results show differences in the distributions of the temperature and the normal current density on the cathode surface and the radial and axial distributions of the plasma temperature. Comparison with the results of a fully non-equilibrium model of the arc plasma and experimental findings from optical emission spect...

Numerical modelling of high-pressure arc discharges: matching the LTE arc core with the electrodes

Journal of Physics D: Applied Physics, 2017

A widely-used approach to simulation of high-pressure arc discharges is based on the system of magneto-hydrodynamic equations written in the approximation of local thermodynamic equilibrium (LTE). In this work, boundary conditions on the surface of the electrodes are formulated with the use of equations of balance of energy in the non-equilibrium near-electrode layers that separate the LTE bulk plasma and the electrodes. As an example, numerical simulations of a free-burning arc in atmospheric-pressure argon plasma in the current range from 20 to 200 A are reported. Simulation results are in a reasonably good agreement with those given by more sophisticated models and with the experiment. Simulations performed for cathodes of slightly different geometries have predicted a strong effect produced by details of the cathode geometry over the distribution of the current density along the cathode surface and therefore over the plasma temperature; an interesting and potentially important result worth of further numerical investigation and experimental verification.

Investigating near-anode plasma layers of very high-pressure arc discharges

Journal of Physics D: Applied Physics, 2009

Numerical and experimental investigation of near-anode layers of very high-pressure arcs in mercury and xenon is reported. The simulation is performed by means of a recently developed numerical model in which the whole of a near-electrode layer is simulated in the framework of a single set of equations without simplifying assumptions such as thermal equilibrium, ionization equilibrium and quasi-neutrality and which was used previously for a simulation of the near-cathode plasma layers. The simulation results support the general understanding of similarities and differences between plasma-cathode and plasma-anode interaction in high-pressure arc discharges established in preceding works. In particular, the anode power input is governed primarily by, and is approximately proportional to, the arc current. In the experiment, the spectral radiance from the electrodes and the near-electrode regions in xenon arcs was recorded. The derived total anode power input and near-anode plasma radiance distribution agree reasonably well with the simulation results.

Characterization of low-pressure arc plasma in large volumes

2017

Study of the large area low-pressure arc discharge plasma in Ar and Ar-N 2 mixtures is presented. The low-pressure arc discharge in large chambers was ignited between planar vacuum arc cathode with magnetic steering of arc spots and surrounding grounded primary anode while long-length remote arc discharge is extended toward remote linear anode parallel to the cathode plate. The arc column was moving up and down perpendicular to the cathode-to-remote anode direction, following the movement of the cathodic arc spots. I-V characteristics of the remote arc discharge were studied by electrophysical measurements. Electron density, electron temperature, and dissociation of nitrogen molecules in the low-pressure DC arc discharge in pure argon and Ar-N 2 mixtures at pressures ranging 1-20 mTorr were studied by electrostatic probes, MW resonant probe, ion energy analyzer and spectral methods at various remote anode currents and gas composition.

Electrical characterization of atmospheric pressure arc plasmas

European Physical Journal D, 2004

The properties of atmospheric pressure arcs are investigated by means of electric exploration of plasma column and anode region. For the electrostatic probe technique, where the level of collisionality distorts the characteristic curve, data interpretation is difficult because no comprehensive underlying theory exists for the non-homogeneous electric arcs used in industry. Results are presented from an extended study of Langmuir probes applied to short, point-plane arcs. A multi-wire apparatus, operating for arc currents in the range 50-200 A is described and ion current densities and temperature maps are shown. The reduction of the probe determined temperature with respect to emission spectroscopy values is discussed and the “cooling” is ascribed to ion-electron recombination within the perturbation region formed around the probe. This region is investigated by means of emission spectroscopy and the extension found agrees both with numerical estimations and fast speed camera photographs. Diamond Like Carbon (DLC) partially coated wires can address data inversion problems and the role of arc flow directionality on charge capture and preliminary observations are shown. Charge capture and anode fall structure can be investigated using a “split-anode” technique. A prototype of a modified apparatus is described and preliminary results on the collected current are given.

The Effect of Argon Pressure on Plate-Shape Electrodes Plasma Forming Behavior

To create plasma, it is needed to introduce some sort of energy into the electrons until reaching the ionization energy, and can be done by heating up the gas or by bombarding of high-energy electromagnetic field using laser or microwave generator. Plasma is ionized gas, i.e. a substance which the electrons excited completely out from the atomic orbit. The main challenge to create a plasma reactor is to develop low gas pressure whilst maintaining high current plasma. Common method used in plasma generating in the industrial world is CCP (capacitive coupled plasma). This method uses a pair of metal electrodes arranged in close distance inside a reactor. The gas pressure inside the reactor is then set to atmospheric pressure or lower. This research analyzes the technique for developing high voltage DC plasma generator in order to supply reactor chamber to generate plasma in low pressure argon environment. Furthermore, this research does the analyzing of breakdown voltage to plot it against gas pressure and distance between electrodes. Making a comparison between experimental plotting and the Paschen Law is the final objective of this research.

Properties of Argon–Nitrogen Atmospheric Pressure DC Arc Plasma

Plasma Chemistry and Plasma Processing, 2015

The effect of nitrogen addition (1-20 %) on atmospheric argon DC arc plasma parameters was investigated. Nitrogen was added to three initial plasma gas compositions: pure argon gas, argon gas with water aerosol, and argon gas with water aerosol containing 0.5 % KCl. Admixtures of nitrogen from 1 up to 10 % (in the case of Ar-N 2-water aerosol plasma) or up to 5 % (in the presence of 0.5 % KCl) produced a more contracted discharge, with larger gradients of electron number density and temperature, as compared to plasma without molecular gas addition. The opposite effect was observed in gas mixtures with 20 % of nitrogen. In that case, the arc core was expanded, and the radial profile of electron density and temperature became flatter as compared to the case of pure argon plasma. The changes in the radial structure of the discharge could be explained by increased thermal conductivity of mixed gas plasma and the presence of molecular ions. Increasing nitrogen content brings plasma closer to thermal equilibrium. To evaluate the effect of nitrogen upon analytic performance of the arc source, limits of detection (LODs) were measured for Zn, Cu, Li, and Rb. In plasma without KCl, the addition of nitrogen resulted in lowering of LODs for Cu, Li and Rb, while the opposite was observed for Zn. In the presence of KCl the addition of nitrogen had little or no effect on LODs for Cu, Li and Rb, while detection limits for Zn were increased. Keywords Atmospheric pressure DC arc discharge Á Argon/nitrogen plasma Á Excitation temperature Á Electron density Á Thermal equilibrium & Jelena Savovic

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