Mode Transition of Filaments in Packed-Bed Dielectric Barrier Discharges

Mingxiang Gao,Hongyu Wang,Bin Guo,Ya Zhang,Quanzhi Zhang,Annemie Bogaerts

doi:10.3390/catal8060248

Mingxiang Gao, Hongyu Wang + Show 4 more

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https://doi.org/10.3390/catal8060248

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Abstract

We investigated the mode transition from volume to surface discharge in a packed bed dielectric barrier discharge reactor by a two-dimensional particle-in-cell/Monte Carlo collision method. The calculations are performed at atmospheric pressure for various driving voltages and for gas mixtures with different N2 and O2 compositions. Our results reveal that both a change of the driving voltage and gas mixture can induce mode transition. Upon increasing voltage, a mode transition from hybrid (volume+surface) discharge to pure surface discharge occurs, because the charged species can escape much more easily to the beads and charge the bead surface due to the strong electric field at high driving voltage. This significant surface charging will further enhance the tangential component of the electric field along the dielectric bead surface, yielding surface ionization waves (SIWs). The SIWs will give rise to a high concentration of reactive species on the surface, and thus possibly enhance the surface activity of the beads, which might be of interest for plasma catalysis. Indeed, electron impact excitation and ionization mainly take place near the bead surface. In addition, the propagation speed of SIWs becomes faster with increasing N2 content in the gas mixture, and slower with increasing O2 content, due to the loss of electrons by attachment to O2 molecules. Indeed, the negative O2− ion density produced by electron impact attachment is much higher than the electron and positive O2+ ion density. The different ionization rates between N2 and O2 gases will create different amounts of electrons and ions on the dielectric bead surface, which might also have effects in plasma catalysis.

Highlights

Plasma catalysis is gaining increasing interest for various environmental applications, such as gaseous pollutant removal, the splitting of CO2, hydrogen generation and O3 production [1,2,3,4,5,6,7,8,9].Plasma catalysis can be regarded as the combination of a plasma with a catalyst, and often results in improved performance, in terms of selectivity and energy efficiency of the process
Plasma catalysis can be realized by introducing dielectric packing beads in the discharge gap, forming a packed bed dielectric barrier discharge (PB-DBD) reactor
The spatial and temporal evolutions of the species densities, electric field, and excitation and ionization rates are presented including the whole process of filament formation and transition to surface ionization waves (SIWs)

Summary

Introduction

Plasma catalysis is gaining increasing interest for various environmental applications, such as gaseous pollutant removal, the splitting of CO2 , hydrogen generation and O3 production [1,2,3,4,5,6,7,8,9]. Plasma catalysis can be regarded as the combination of a plasma with a catalyst, and often results in improved performance, in terms of selectivity and energy efficiency of the process. Plasma is an ionized gas, consisting of various reactive species, like electrons, positive ions, negative ions and radicals. These reactive species are created by applying a potential difference to a gas. Each streamer starts when the driving voltage passes a certain threshold, and will further polarize the dielectric surface [20]

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