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On modeling of “plasmoid” created by electric discharge

The result's identifiers

  • Result code in IS VaVaI

    <a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F61389021%3A_____%2F18%3A00498228" target="_blank" >RIV/61389021:_____/18:00498228 - isvavai.cz</a>

  • Result on the web

    <a href="http://iopscience.iop.org/article/10.1088/1742-6596/996/1/012012/meta" target="_blank" >http://iopscience.iop.org/article/10.1088/1742-6596/996/1/012012/meta</a>

  • DOI - Digital Object Identifier

    <a href="http://dx.doi.org/10.1088/1742-6596/996/1/012012" target="_blank" >10.1088/1742-6596/996/1/012012</a>

Alternative languages

  • Result language

    angličtina

  • Original language name

    On modeling of “plasmoid” created by electric discharge

  • Original language description

    Plasma processes involving liquid phases are widely used in various applications, such as biomedical processes, shock wave generation for medical applications, material processes, sterilization in water treatment and others. Two main configurations of high voltage electrodes submersed in water have been used for an electrical discharge generation: pin˗to˗pin and pin˗to˗plate. An electrical breakdown in the plate˗to˗plate configuration is generally difficult to reproduce, because there is a uniform and weak electric field in the interelectrode region in this geometry. One major advantage of using plate electrodes is their greater “wear hardness” to high-energy discharges. The plate electrodes can withstand extremely high energy deposition at which the pin electrode is quickly destroyed. Due to that the system of plate electrodes is proposed to be used for shock wave generation in litotripsy. The electrical discharge between plate electrodes can be initiated by creating an inhomogeneity in the electrical field. Two methods of discharge initiation between plate electrodes are proposed for this aim: 1) focusing of a shock wave in the interelectrode region, 2) a bubble injection into the electrode gap. Both methods employ the fact that a typical order of magnitude of an electrical breakdown field for gas is 30 kV cm−1 , i.e. 30 times less than the electrical field required for the electrical breakdown in water. The physical mechanisms of discharge initiation and positive streamer propagation are discussed.

  • Czech name

  • Czech description

Classification

  • Type

    D - Article in proceedings

  • CEP classification

  • OECD FORD branch

    10305 - Fluids and plasma physics (including surface physics)

Result continuities

  • Project

  • Continuities

    I - Institucionalni podpora na dlouhodoby koncepcni rozvoj vyzkumne organizace

Others

  • Publication year

    2018

  • Confidentiality

    S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů

Data specific for result type

  • Article name in the collection

    Journal of Physics: conference series

  • ISBN

  • ISSN

    1742-6588

  • e-ISSN

  • Number of pages

    7

  • Pages from-to

  • Publisher name

    Institute of physics

  • Place of publication

    Bristol

  • Event location

    Moskva

  • Event date

    Nov 22, 2017

  • Type of event by nationality

    WRD - Celosvětová akce

  • UT code for WoS article

    000445819900012