Abstract

The plasma behavior in a parallel-plate dielectric barrier discharge (DBD) is simulated by a two-dimensional particle-in-cell/Monte Carlo collision model, comparing for the first time an unpacked (empty) DBD with a packed bed DBD, i.e., a DBD filled with dielectric spheres in the gas gap. The calculations are performed in air, at atmospheric pressure. The discharge is powered by a pulse with a voltage amplitude of −20 kV. When comparing the packed and unpacked DBD reactors with the same dielectric barriers, it is clear that the presence of the dielectric packing leads to a transition in discharge behavior from a combination of negative streamers and unlimited surface streamers on the bottom dielectric surface to a combination of predominant positive streamers and limited surface discharges on the dielectric surfaces of the beads and plates. Furthermore, in the packed bed DBD, the electric field is locally enhanced inside the dielectric material, near the contact points between the beads and the plates, and therefore also in the plasma between the packing beads and between a bead and the dielectric wall, leading to values of V m−1, which is much higher than the electric field in the empty DBD reactor, i.e., in the order of V m−1, thus resulting in stronger and faster development of the plasma, and also in a higher electron density. The locally enhanced electric field and the electron density in the case of a packed bed DBD are also examined and discussed for three different dielectric constants, i.e., (ZrO2), (Al2O3) and (SiO2). The enhanced electric field is stronger and the electron density is higher for a larger dielectric constant, because the dielectric material is more effectively polarized. These simulations are very important, because of the increasing interest in packed bed DBDs for environmental applications.

Highlights

  • Dielectric barrier discharges (DBDs) at atmospheric pressure [1,2,3,4] usually occur in the filamentary regime in most gases [5]

  • Photoionization might be important in the mechanism of streamer formation [17], it is not taken into account in this model, because in a packed bed DBD, the photons cannot travel freely like in an unpacked DBD, as the gas gap spacing is small and the geometry is complex, so most photons will more likely be lost at the surface of the dielectric beads instead of contributing to ionization

  • We have presented a 2D particle-in cell/Monte Carlo collision (PIC/MCC) model, obtained with the VSim simulation code, to study the properties of both negative and positive streamers in an atmospheric pressure DBD operating in air, comparing an unpacked and a packed bed DBD reactor in the filamentary regime, with an applied voltage of −20 kV and a gap size of 1 mm

Read more

Summary

27 August 2015

The plasma behavior in a parallel-plate dielectric barrier discharge (DBD) is simulated by a twoand DOI. The locally enhanced electric field and the electron density in the case of a packed bed DBD are examined and discussed for three different dielectric constants, i.e., r = 22 (ZrO2), r = 9 (Al2O3) and r = 4 (SiO2). The enhanced electric field is stronger and the electron density is higher for a larger dielectric constant, because the dielectric material is more effectively polarized. These simulations are very important, because of the increasing interest in packed bed DBDs for environmental applications

Introduction
Simulation Model and Conditions
Results and discussion
Conclusion
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.