The dataset provides the data related to the modelling of microdischarges in metal vapour of cadmium and zinc. The characterisation of the microdischarges was done in a framework that combined a unified nonequilibrium plasma model and a collisional-radiative model. The plasma model provided the basic plasma parameters (number densities of ground state neutral and singly charged species and their energies, electric field, discharge voltage). Number densities of excited atomic states were obtained on a second stage employing a collisional-radiative model and the already known plasma parameters. This modelling framework allowed one to obtain spatially and temporally resolved plasma parameters and the population of the excited atomic states in the entire discharge gap during the separation of the electric contacts. The modelling work was supported by electrical measurements, high-speed imaging and optical emission spectroscopy. The experimental findings enabled the calibration of the plasma model with respect to the discharge voltage and a qualitative and to some extent quantitative comparison of computed and measured spectral intensities.
| Field | Value |
|---|---|
| Group | |
| Authors | |
| Release Date | 2026-05-27 |
| Identifier | d8420686-6b4f-40b9-b02d-2e13b4e3c08a |
| Permanent Identifier (DOI) | |
| Permanent Identifier (URI) | |
| Plasma Source Name | |
| Plasma Source Application | |
| Plasma Source Specification | |
| Plasma Source Properties | The electrode configuration includes a cathode made of cadmium (Cd) and zinc (Zn) and an anode made of tungsten (W) with lengths of 10mm and a diameter of 100 μm each. The length of the plasma region varies from 20 μm up to 160 μm during the contact separation. |
| Plasma Source Procedure | An electric contact of a wire (anode) is established on the rough surface of a metal block (cathode). The wire is pulled away from the surface which initiates an electric discharge. The main discharge develops in metal vapour at distances between 20 μm and ∼ 200 μm (the so-called microdischarges). The wire moves further away from the surface, the released heat causes a thermochemical reaction, which can lead to the formation and the development of a flame front. |
| Plasma Medium Name | |
| Plasma Medium Properties | The plasma is assumed to contain electrons and heavy particles of Cd or Zn atoms and singly charged Cd+ or Zn+ ions in their ground states. Admixture of air/H2 appears after the main microdischarge. |
| Plasma Medium Procedure | Spark ignition occurs during the contact separation at a constant current of 60 mA. Initially, the spark is ignited in the metal vapour of Cd or Zn. Later on the gas characterising the explosive atmopshere (a mixture air/H2) is supposed to mix with the metal vapour. |
| Plasma Target Name | |
| Plasma Target Properties | Melting and evaporation of the cathode made of Cd or Zn. Thermo-field emission from the Cd/Zn cathode with precomputed values of the electric current density as a function of the electric field and the temperature on the cathode |
| Plasma Diagnostics Name | |
| Plasma Diagnostics Properties | A framework that combines a unified nonequilibrium plasma model and a collisional-radiative model is employed. The plasma model provides the basic plasma parameters (number densities of ground state neutral and singly charged species and their energies, electric field, discharge voltage). Number densities of excited atomic states were obtained on a second stage employing a collisional-radiative model and the already known plasma parameters. This modelling framework allowed one to obtain spatially and temporally resolved plasma parameters and the population of the excited atomic states in the entire discharge gap during the separation of the electric contacts. |
| Plasma Diagnostics Procedure | The model equations are solved using a fully coupled approach. The electric current in the model has a constant value of 60mA. A steady-state solution is sought for a gap length of 20 μm to mimic the initial two phases of contact opening. Then, a deforming mesh approach is applied to simulate the moving electrode. The discharge gap was increased from 20 μm up to 160 μm with a speed of 0.14m/s. |
| Language | English |
| License | |
| Public Access Level | Public |
| Contact Name | Baeva, Margarita |
| Contact Email |
Data and Resources
- Framework of unified nonequilibrium plasma model and collisional-radiative model - Ionisation rate coefficients (figure 1)csv
Ionisation rate coefficients Kion,t [m^3/s] for Cd and Zn as a function of...
Preview Download - Framework of unified nonequilibrium plasma model and collisional-radiative model - Thermo-field emission current density of electrons from a cathode made of Cd (figure 2a)csv
Thermo-field emission current density of electrons jtf [A/m^2] from a...
Preview Download - Framework of unified nonequilibrium plasma model and collisional-radiative model - Thermo-field emission current density of electrons from a cathode made of Zn (figure 2b)csv
Thermo-field emission current density of electrons jtf [A/m^2] from a...
Preview Download - Framework of unified nonequilibrium plasma model and collisional-radiative model - Measured and computed in the UNEM voltage for microdischarges in metal vapours of Cd (figure 4a)csv
Measured and computed in the UNEM voltage for microdischarges with gap...
Preview Download - Framework of unified nonequilibrium plasma model and collisional-radiative model - Measured and computed in the UNEM voltage for microdischarges in metal vapours of Zn (figure 4b)csv
Measured and computed in the UNEM voltage for microdischarges with gap...
Preview Download - Framework of unified nonequilibrium plasma model and collisional-radiative model - Distributions of the electric potential for microdischarges in metal vapours of Cd (figure 5 Cd)csv
Distributions of the electric potential for microdischarges with gap lengths...
Preview Download - Framework of unified nonequilibrium plasma model and collisional-radiative model - Distributions of the electric potential for microdischarges in metal vapours of Zn (figure 5 Zn)csv
Distributions of the electric potential for microdischarges with gap lengths...
Preview Download - Framework of unified nonequilibrium plasma model and collisional-radiative model - Density of space charge in the vicinity of the cathode in microdischarges of Cd (figure 6 Cd)csv
Spatial distribution of the space charge density in the cathode sheath of...
Preview Download - Framework of unified nonequilibrium plasma model and collisional-radiative model - Density of space charge in the vicinity of the cathode in microdischarges of Zn (figure 6 Zn)csv
Spatial distribution of the space charge density in the cathode sheath of...
Preview Download - Framework of unified nonequilibrium plasma model and collisional-radiative model - Distribution of the electron temperature in microdischages of metal vapour of Cd and Zn (figure 7a)csv
Distribution of the electron temperature Te in microdischages of metal...
Preview Download - Framework of unified nonequilibrium plasma model and collisional-radiative model - Distributions of the gas temperature in microdischages of metal vapour of Cd and Zn (figure 7b)csv
Distributions of the gas temperature T in microdischages of metal vapour of...
Preview Download - Framework of unified nonequilibrium plasma model and collisional-radiative model - Predicted number densities of electrons and excited states of Cd and Zn (figure 8)csv
Predicted number densities of electrons and excited states of Cd and Zn for...
Preview Download - Framework of unified nonequilibrium plasma model and collisional-radiative model - Temporal evolution of the spatially averaged line intensities in Cd (figure 9a)csv
Temporal evolution of the spatially averaged line intensities Iqp(λ, t) in...
Preview Download - Framework of unified nonequilibrium plasma model and collisional-radiative model - Temporal evolution of the spatially averaged line intensities in Zn (figure 9b)csv
Temporal evolution of the spatially averaged line intensities Iqp(λ, t) in...
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