4.6 Article

Thermal and hydrodynamic effects of nanosecond discharges in atmospheric pressure air

期刊

出版社

IOP PUBLISHING LTD
DOI: 10.1088/0022-3727/47/23/235202

关键词

ultrafast heating; nanosecond discharges; schlieren

资金

  1. Agence Nationale de la Recherche PREPA project [ANR-09-BLAN-0043]
  2. PLASMAFLAME project [ANR-11-BS09-025-01]
  3. Erasmus Mundus Tandem Program
  4. Agence Nationale de la Recherche (ANR) [ANR-09-BLAN-0043] Funding Source: Agence Nationale de la Recherche (ANR)

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We present quantitative schlieren measurements and numerical analyses of the thermal and hydrodynamic effects of a nanosecond repetitively pulsed (NRP) discharge in atmospheric pressure air at 300 and 1000 K. The plasma is created by voltage pulses at an amplitude of 10 kV and a duration of 10 ns, applied at a frequency of 1-10 kHz between two pin electrodes separated by 2 or 4 mm. The electrical energy of each pulse is of the order of 1 mJ. We recorded single-shot schlieren images starting from 50 ns to 3 mu s after the discharge. The time-resolved images show the shock-wave propagation and the expansion of the heated gas channel. Gas density profiles simulated in 1D cylindrical coordinates have been used to reconstruct numerical schlieren images for comparison with experimental ones. We propose an original method to determine the initial gas temperature and the fraction of energy transferred into ultrafast gas heating, using a comparison of the contrast profiles obtained from experimental and numerical schlieren images. This method is found to be much more sensitive to these parameters than the direct comparison of measured and predicted shock-wave and heated channel radii. The results show that a significant fraction of the electric energy is converted into gas heating within a few tens of ns. The values range from about 25% at a reduced electric field of 164 Td to about 75% at 270 Td, with a strong dependance on the initial gas temperature. These experiments support the fast heating processes via dissociative quenching of N-2(B-3 Pi(g), C-3 Pi(u)) by molecular oxygen.

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