TY - JOUR
T1 - Pulsed microplasmas generated in truncated paraboloidal microcavities
T2 - Simulations of particle densities and energy flow
AU - Lee, H. J.
AU - Park, S. J.
AU - Eden, J. G.
N1 - One of the authors (T.S.) is very grateful to the Alexander von Humboldt Foundation (Germany) and to the Ministry of Education, Culture and Sports of Spain for the financial support.
PY - 2012/10/10
Y1 - 2012/10/10
N2 - Microplasmas generated within cavities having the form of a truncated paraboloid, introduced by Kim et al (2009 Appl. Phys. Lett. 94 011503), have been simulated numerically with a two-dimensional, fluid computational model. Microcavities with parabolic sidewalls, fabricated in nanoporous alumina (Al 2O 3) and having upper (primary emitter) and lower apertures of 150m and 75m in diameter, respectively, are driven by a bipolar voltage waveform at a frequency of 200kHz. For a Ne pressure of 500Torr and 2s, 290V pulses constituting each half-cycle of the driving voltage waveform, calculations predict that 10nJ of energy is delivered to each parabolic cavity, of which 26-30% is consumed by the electrons. Once the cathode fall is formed, approximately 65% and 8% of the input energy is devoted to driving the atomic ion and dimer ion currents, respectively, and the peak electron density of 6×10 12cm 3 is attained 90ns following the onset of the first half-cycle (positive) voltage pulse. Specific power loading of the microplasma reaches 150kWcm 3 and the loss of power to the wall of the microcavity drops by as much as 24% when the excitation voltage is increased from 280 to 310V. The diminished influence of diffusion with increasing pressure is responsible for wall losses at 600Torr accounting for <20% of the total electron energy.
AB - Microplasmas generated within cavities having the form of a truncated paraboloid, introduced by Kim et al (2009 Appl. Phys. Lett. 94 011503), have been simulated numerically with a two-dimensional, fluid computational model. Microcavities with parabolic sidewalls, fabricated in nanoporous alumina (Al 2O 3) and having upper (primary emitter) and lower apertures of 150m and 75m in diameter, respectively, are driven by a bipolar voltage waveform at a frequency of 200kHz. For a Ne pressure of 500Torr and 2s, 290V pulses constituting each half-cycle of the driving voltage waveform, calculations predict that 10nJ of energy is delivered to each parabolic cavity, of which 26-30% is consumed by the electrons. Once the cathode fall is formed, approximately 65% and 8% of the input energy is devoted to driving the atomic ion and dimer ion currents, respectively, and the peak electron density of 6×10 12cm 3 is attained 90ns following the onset of the first half-cycle (positive) voltage pulse. Specific power loading of the microplasma reaches 150kWcm 3 and the loss of power to the wall of the microcavity drops by as much as 24% when the excitation voltage is increased from 280 to 310V. The diminished influence of diffusion with increasing pressure is responsible for wall losses at 600Torr accounting for <20% of the total electron energy.
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U2 - 10.1088/0022-3727/45/40/405201
DO - 10.1088/0022-3727/45/40/405201
M3 - Article
AN - SCOPUS:84866868941
SN - 0022-3727
VL - 45
JO - Journal of Physics D: Applied Physics
JF - Journal of Physics D: Applied Physics
IS - 40
M1 - 405201
ER -