Study of the dielectric breakdown strength of CO2–O2 mixtures by considering ion kinetics in a spatial–temporal growth avalanche model

The gas mixture CO2–O2 has been considered as an insulation and arc-quenching medium in gas-insulated switchgears. In this paper, the dielectric breakdown properties of CO2–O2 mixtures at different O2 concentrations and gas pressures were studied theoretically by considering ion kinetics in a spatial–temporal growth avalanche model. A kinetic scheme that includes all the main reactions likely to occur in CO2–O2 mixtures is presented. An improved method to calculate the dielectric strength of the gas mixture is developed, based on an avalanche model that considers both spatial growth and temporal processes. Next, the reaction rates of ionization, attachment, detachment and ion conversion, the effective ionization Townsend coefficient αeff/N, and reduced critical electric field strength ( E/N) cr in CO2–O2 mixtures at different mixing ratios and gas pressures are analyzed in detail. Finally, a pulsed Townsend experiment is performed to verify the validity and accuracy of the calculation method. Based on this, one detachment reaction rate is modified to yield more accurate results. Better consistency between the results and the experimental values supports the validity of the kinetic system, reaction rates, and the improved calculation method.

[1]  A. Murphy,et al.  Pulsed Townsend measurement of electron swarm parameters in C4F7N–CO2 and C4F7N–N2 mixtures as eco-friendly insulation gas , 2022, Journal of Applied Physics.

[2]  Boya Zhang,et al.  Electron swarm parameters and dielectric strength of C5F10O and its mixtures with CO2 and dry air , 2021, Journal of Physics D: Applied Physics.

[3]  A. Murphy,et al.  Fundamental physicochemical properties of SF6-alternative gases: a review of recent progress , 2020, Journal of Physics D: Applied Physics.

[4]  Y. Yokomizu,et al.  Chemical species produced in arc-quenching gas CO2/O2 mixed with C3H2F4, C4-FN or C5-FK: prevention of condensed-phase carbon formation and its formulation , 2020, Journal of Physics D: Applied Physics.

[5]  Di-bo Wang,et al.  Effect of humidity on dielectric breakdown properties of air considering ion kinetics , 2018, Journal of Physics D: Applied Physics.

[6]  C. Franck,et al.  Experimentally derived rate coefficients for electron ionization, attachment and detachment as well as ion conversion in pure O2 and N2–O2 mixtures , 2018, Journal of Physics D: Applied Physics.

[7]  A. Murphy,et al.  SF6-alternative gases for application in gas-insulated switchgear , 2018 .

[8]  Xingwen Li,et al.  Study of the dielectric breakdown properties of CO2–O2 mixtures by considering electron detachments from negative ions , 2017 .

[9]  A. Bogaerts,et al.  Effective ionisation coefficients and critical breakdown electric field of CO2 at elevated temperature: effect of excited states and ion kinetics , 2016 .

[10]  Hu Zhao,et al.  Dielectric breakdown properties of N2–O2 mixtures by considering electron detachments from negative ions , 2016 .

[11]  M. Rong,et al.  Determination of the Dominant Species and Reactions in Non-equilibrium CO2 Thermal Plasmas with a Two-Temperature Chemical Kinetic Model , 2016, Plasma Chemistry and Plasma Processing.

[12]  S. Jia,et al.  Prediction of the critical reduced electric field strength for carbon dioxide and its mixtures with copper vapor from Boltzmann analysis for a gas temperature range of 300 K to 4000 K at 0.4 MPa , 2015 .

[13]  Haonan Sun,et al.  Influence of O2 on the dielectric properties of CO2 at the elevated temperatures , 2014 .

[14]  S. Jia,et al.  Prediction of the critical reduced electric field strength for carbon dioxide and its mixtures with 50% O2 and 50% H2 from Boltzmann analysis for gas temperatures up to 3500 K at atmospheric pressure , 2014 .

[15]  S. Pancheshnyi Effective ionization rate in nitrogen–oxygen mixtures , 2013 .

[16]  Christian M. Franck,et al.  Obtaining precise electron swarm parameters from a pulsed Townsend setup , 2012 .

[17]  S. Jia,et al.  Dielectric breakdown properties of SF6–N2 mixtures in the temperature range 300–3000 K , 2012 .

[18]  A. Bogaerts,et al.  Influence of Vibrational States on CO2 Splitting by Dielectric Barrier Discharges , 2012 .

[19]  O. Ducasse,et al.  Determination of transport and reaction swarm coefficients from the analysis of complex transient pulses from the pulsed Townsend experiment , 2012 .

[20]  L. Pitchford,et al.  Solving the Boltzmann equation to obtain electron transport coefficients and rate coefficients for fluid models , 2005 .

[21]  James K. Olthoff,et al.  Sulfur hexafluoride and the electric power industry , 1997 .

[22]  S. Lawton,et al.  Excitation of the b 1Σ+g state of O2 by low energy electrons , 1978 .

[23]  F. Fehsenfeld,et al.  Laboratory studies of negative ion reactions with atmospheric trace constituents , 1974 .

[24]  G. S. Hurst,et al.  Determination of Electron‐Capture Cross Sections with Swarm‐Beam Techniques , 1965 .

[25]  J. Craggs,et al.  Measurement of Ionization and Attachment Coefficients in Carbon Dioxide in Uniform Fields , 1960 .