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
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Czech description
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Classification
Type
D - Article in proceedings
CEP classification
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OECD FORD branch
10305 - Fluids and plasma physics (including surface physics)
Result continuities
Project
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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
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ISSN
1742-6588
e-ISSN
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Number of pages
7
Pages from-to
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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