z-logo
open-access-imgOpen Access
Nanosecond pulsed discharges in distilled water-Part II: line emission and plasma propagation
Author(s) -
Achim von Keudell,
Katharina Grosse,
Volker Schulz-von der Gathen
Publication year - 2020
Publication title -
plasma sources science and technology
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.9
H-Index - 108
eISSN - 1361-6595
pISSN - 0963-0252
DOI - 10.1088/1361-6595/aba4b9
Subject(s) - plasma , nanosecond , atomic physics , ionization , emission spectrum , stark effect , plasma diagnostics , chemistry , tungsten , electron density , absorption (acoustics) , spectral line , analytical chemistry (journal) , ion , laser , optics , physics , chromatography , astronomy , organic chemistry , quantum mechanics
Nanosecond plasmas in liquids can initiate chemical processes that are exploited in the fields of water treatment, electrolysis or biomedical applications. The understanding of these chemical processes relies on unraveling the dynamics of the variation of pressures, temperatures and species densities during the different stages of plasma ignition and plasma propagation as well as the conversion of the liquid into the plasma state and the gas phase. This is analyzed by monitoring the emission of nanosecond pulsed plasmas that are generated by high voltages of 20 kV and pulse lengths of 10 ns applied to a tungsten tip with 50 μ m diameter immersed in water. The spectra are acquired with a temporal resolution of 2 ns and the emission pattern is modelled by a combination of black body radiation from the hot tungsten tip and the pronounced emission lines of the hydrogen Balmer series. The data indicate two contributions of the hydrogen line radiation that differ with respect to the degree of self-absorption. It is postulated that one contribution originates from a recombination region showing strong self absorption and one contribution from an ionization region showing very little self-absorption. The emission lines from the ionization region are evaluated assuming Stark broadening, that yielded electron densities up to 5 × 10 25  m −3 . The electron density evolution follows the same trend as the temporal evolution of the voltage applied to the tungsten tip. The propagation mechanism of the plasma is similar to that of a positive streamer in the gas phase, although in the liquid phase field effects such as electron transport by tunneling should play an important role.

The content you want is available to Zendy users.

Already have an account? Click here to sign in.
Having issues? You can contact us here