In this work we present for the first time a unified model of a low-current short-length arc between copper electrodes. The model employs one-dimensional fluid description of the plasma in argon and copper vapour at atmospheric pressure and the heat transfer in the electrodes made of copper. The solution of the particle and energy conservation of electrons and heavy particles is coupled with the solution of the Poisson equation, from which the self-consistent electric field is obtained. The operation of the non-refractory cathode is based on thermo-field emission. Heat fluxes from the plasma to the electrodes are considered so that a phase change and evaporation from the cathode and a release of copper atoms into the plasma are taken into account. The influence of the copper atoms and ions on the plasma properties is analysed and discussed. The model's predictions are compared with experimental data and a qualitative agreement is obtained besides the restrictions of the one-dimensional fluid model.
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Authors | |
Release Date | 2020-08-12 |
Identifier | bac1c563-e56f-4fa4-b505-0ceb415f4239 |
Permanent Identifier (DOI) | |
Permanent Identifier (URI) | |
Is supplementing | |
Plasma Source Name | |
Plasma Source Specification | |
Plasma Source Properties | Electrodes made of copper, cylindrical rods with a length of 20 mm and a radius of 2 mm. The arc is ignited in argon (laminar flow with a flow rate of 6.5 slm) at atmopsheric pressure. Arc current 3.5 A. Copper atoms enter the plasma due to melting of the electrodes. |
Plasma Medium Name | |
Plasma Medium Properties | The plasma is in non-equilibrium. |
Plasma Diagnostics Name | |
Plasma Diagnostics Properties | A monochromator (MDR-12) with a CCD linear image sensor (B/W) (3000-pixels, Sony ILX526A) provides a fast scan of the spatial distribution of the radial intensity. |
Plasma Diagnostics Procedure | Integration over the wavelength interval is performed and the side-on observations are transformed via Abel inversion to give the radial dependence of the emission coefficient. The Boltzmann plot technique is applied to determine the excitation temperature. |
Language | English |
License | |
Public Access Level | Public |
Contact Name | Baeva, Margarita |
Contact Email |
Data and Resources
- Short-length arcs between copper electrodes_Fig.1csv
The calculated current density due to thermo-field emission of electrons...
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Boltzmann plots for three radial positions in the midplane of the arc at arc...
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Radial distribution of the excitation temperature T in the midplane of the...
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Predicted properties as a function of the field enhancement factor and a...
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Predicted properties as a function of the current density for FEF=200 in...
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Predicted plasma composition as a function of the current density for FEF=...
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The electron density as a function of the current density in pure argon for...
Preview Download - Short-length arcs between copper electrodes_Fig.8_1csv
Predicted plasma parameters along the interelectrode distance for FEF=200 at...
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Predicted plasma parameters along the interelectrode distance for FEF=200 at...
Preview Download - Short-length arcs between copper electrodes_Fig.9acsv
a) Spectral emission coeffcient for the radiative transition considered in...
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b) Spectral emission coeffcient for the radiative transition considered in...
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