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Underwater Electrical Discharge with a Large Surface of Radiation
Breakdown and formation of surface electric discharge in a zone of turbulent agitation of water jet transverse to the axis of an electrode system are studied. The jet boundary is actually a two-phase medium favorable for electron breeding consisting of cavitation microbubbles up to 10 7 cm -3 in vol...
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Published in: | IEEE transactions on dielectrics and electrical insulation 2007-10, Vol.14 (5), p.1291-1294 |
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container_title | IEEE transactions on dielectrics and electrical insulation |
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creator | Azizov, E.A. Emelyanov, A.I. Yagnov, V.A. |
description | Breakdown and formation of surface electric discharge in a zone of turbulent agitation of water jet transverse to the axis of an electrode system are studied. The jet boundary is actually a two-phase medium favorable for electron breeding consisting of cavitation microbubbles up to 10 7 cm -3 in volume. These features differentiate the considered discharge from a low-voltage breakdown in a stationary liquid. Abnormal properties of electric discharge in a submerged water stream take place both at the initiation and at the stationary stage. The threshold voltages are reduced by several times at the stream velocities of about 30 m/s, simultaneously the duration of the prebreakdown stage is reduced by one to two orders of magnitude. At the arc stage of the discharge, there is a developed emitting surface with plasma shell thickness being about 1 mm. The change of initial water conductivity by four orders of magnitude does not lead to large changes in breakdown dynamics. |
doi_str_mv | 10.1109/TDEI.2007.4339491 |
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The jet boundary is actually a two-phase medium favorable for electron breeding consisting of cavitation microbubbles up to 10 7 cm -3 in volume. These features differentiate the considered discharge from a low-voltage breakdown in a stationary liquid. Abnormal properties of electric discharge in a submerged water stream take place both at the initiation and at the stationary stage. The threshold voltages are reduced by several times at the stream velocities of about 30 m/s, simultaneously the duration of the prebreakdown stage is reduced by one to two orders of magnitude. At the arc stage of the discharge, there is a developed emitting surface with plasma shell thickness being about 1 mm. The change of initial water conductivity by four orders of magnitude does not lead to large changes in breakdown dynamics.</description><identifier>ISSN: 1070-9878</identifier><identifier>EISSN: 1558-4135</identifier><identifier>DOI: 10.1109/TDEI.2007.4339491</identifier><identifier>CODEN: ITDIES</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>Breakdown ; Breakdown voltage ; Cavitation ; Circuits ; Conductivity ; Electric arcs ; Electric breakdown ; Electric discharges ; Electrodes ; Fault location ; Freshwater ; Microorganisms ; Plasma measurements ; Streams ; Surface discharges ; Threshold voltage ; Water</subject><ispartof>IEEE transactions on dielectrics and electrical insulation, 2007-10, Vol.14 (5), p.1291-1294</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. 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The jet boundary is actually a two-phase medium favorable for electron breeding consisting of cavitation microbubbles up to 10 7 cm -3 in volume. These features differentiate the considered discharge from a low-voltage breakdown in a stationary liquid. Abnormal properties of electric discharge in a submerged water stream take place both at the initiation and at the stationary stage. The threshold voltages are reduced by several times at the stream velocities of about 30 m/s, simultaneously the duration of the prebreakdown stage is reduced by one to two orders of magnitude. At the arc stage of the discharge, there is a developed emitting surface with plasma shell thickness being about 1 mm. The change of initial water conductivity by four orders of magnitude does not lead to large changes in breakdown dynamics.</description><subject>Breakdown</subject><subject>Breakdown voltage</subject><subject>Cavitation</subject><subject>Circuits</subject><subject>Conductivity</subject><subject>Electric arcs</subject><subject>Electric breakdown</subject><subject>Electric discharges</subject><subject>Electrodes</subject><subject>Fault location</subject><subject>Freshwater</subject><subject>Microorganisms</subject><subject>Plasma measurements</subject><subject>Streams</subject><subject>Surface discharges</subject><subject>Threshold voltage</subject><subject>Water</subject><issn>1070-9878</issn><issn>1558-4135</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2007</creationdate><recordtype>article</recordtype><recordid>eNqFkU1Lw0AQhoMoWKs_QLwED-oldWY_kt1jaasWCoLW87LZbGxK2tRNQvHfu7HVg4d6mq9nXoZ5g-ASYYAI8n4-nkwHBCAZMEolk3gU9JBzETGk_NjnkEAkRSJOg7O6XgIg4yTuBcO3dWbdVjfWhZPSmsYVRpfhuKjNQrt3G26LZhHqcPZdvLYu18aGVR6-6KzQTVGtz4OTXJe1vdjHfjB_mMxHT9Hs-XE6Gs4iwwg0kYwZCBljTEkiU2IpMMhS37DACImZyFKeZsRQyjOt45xKznNMwEhLkjyn_eB2J7tx1Udr60at_I22LPXaVm2tJFAvDYz_S3ZXCCFQePLmIEkZo0LK2IN3B0FMKCCQRHSa13_QZdW6tf-MkkgIQ47UQ7iDjKvq2tlcbVyx0u5TIajOT9X5qTo_1d5Pv3O12ymstb_8z_QLVfeYKw</recordid><startdate>20071001</startdate><enddate>20071001</enddate><creator>Azizov, E.A.</creator><creator>Emelyanov, A.I.</creator><creator>Yagnov, V.A.</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. 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The jet boundary is actually a two-phase medium favorable for electron breeding consisting of cavitation microbubbles up to 10 7 cm -3 in volume. These features differentiate the considered discharge from a low-voltage breakdown in a stationary liquid. Abnormal properties of electric discharge in a submerged water stream take place both at the initiation and at the stationary stage. The threshold voltages are reduced by several times at the stream velocities of about 30 m/s, simultaneously the duration of the prebreakdown stage is reduced by one to two orders of magnitude. At the arc stage of the discharge, there is a developed emitting surface with plasma shell thickness being about 1 mm. The change of initial water conductivity by four orders of magnitude does not lead to large changes in breakdown dynamics.</abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/TDEI.2007.4339491</doi><tpages>4</tpages></addata></record> |
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source | IEEE Electronic Library (IEL) Journals |
subjects | Breakdown Breakdown voltage Cavitation Circuits Conductivity Electric arcs Electric breakdown Electric discharges Electrodes Fault location Freshwater Microorganisms Plasma measurements Streams Surface discharges Threshold voltage Water |
title | Underwater Electrical Discharge with a Large Surface of Radiation |
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