TY - JOUR
T1 - Experiments and simulations of an atmospheric pressure lossy dielectric barrier Townsend discharge
AU - Im, S.
AU - Bak, M. S.
AU - Hwang, N.
AU - Cappelli, M. A.
PY - 2014/2/26
Y1 - 2014/2/26
N2 - A diffuse discharge is produced in atmospheric pressure air between porous alumina dielectric barriers using low-frequency (60 Hz) alternating current. To study its formation mechanism, both the discharge current and voltage are measured while varying the dielectric barrier porosity (0%, 48% or 85%) and composition (99% Al2O3,99% SiO2 or 75% Al 2O3 + 16% SiO2 + 9% other oxides). Time-resolved imaging of the emission is carried out to understand the discharge structure. The results indicate that the ionization is driven by an electron avalanche process. This Townsend discharge is found to persist for quite some time (∼3 ms) when the barriers are alumina with a high porosity (>48%). Micro-streamers are observed for the low porosity alumina barriers as well as for other oxide barriers. This discharge formation with highly porous alumina in air is attributed to a relatively low volume dielectric barrier resistivity (∼105 Ω m). Simulations are carried out, accounting for the surface charge loss due to this porosity, as well as for charge accumulation at the barriers.
AB - A diffuse discharge is produced in atmospheric pressure air between porous alumina dielectric barriers using low-frequency (60 Hz) alternating current. To study its formation mechanism, both the discharge current and voltage are measured while varying the dielectric barrier porosity (0%, 48% or 85%) and composition (99% Al2O3,99% SiO2 or 75% Al 2O3 + 16% SiO2 + 9% other oxides). Time-resolved imaging of the emission is carried out to understand the discharge structure. The results indicate that the ionization is driven by an electron avalanche process. This Townsend discharge is found to persist for quite some time (∼3 ms) when the barriers are alumina with a high porosity (>48%). Micro-streamers are observed for the low porosity alumina barriers as well as for other oxide barriers. This discharge formation with highly porous alumina in air is attributed to a relatively low volume dielectric barrier resistivity (∼105 Ω m). Simulations are carried out, accounting for the surface charge loss due to this porosity, as well as for charge accumulation at the barriers.
KW - dielectric barrier discharge
KW - high pressure glow discharge
KW - porous dielectric barrier
UR - https://www.scopus.com/pages/publications/84894444080
U2 - 10.1088/0022-3727/47/8/085202
DO - 10.1088/0022-3727/47/8/085202
M3 - Article
AN - SCOPUS:84894444080
SN - 0022-3727
VL - 47
JO - Journal of Physics D: Applied Physics
JF - Journal of Physics D: Applied Physics
IS - 8
M1 - 085202
ER -