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The process of commutation of small vacuum gaps with initiation by an electric spark plasma and laser plasma
For a vacuum spark gap with initiation by an electric spark plasma, the limited possibilities of controlling the delay time of switching by varying the energy of the auxiliary discharge are demonstrated. For a vacuum spark gap with initiation by a laser plasma, the threshold value of the radiation e...
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Published in: | High temperature 2017-03, Vol.55 (2), p.191-198 |
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container_title | High temperature |
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creator | Asyunin, V. I. Davydov, S. G. Dolgov, A. N. Kozlovskaya, T. I. Revazov, V. O. Seleznev, V. P. Yakubov, R. H. |
description | For a vacuum spark gap with initiation by an electric spark plasma, the limited possibilities of controlling the delay time of switching by varying the energy of the auxiliary discharge are demonstrated. For a vacuum spark gap with initiation by a laser plasma, the threshold value of the radiation energy is detected at which the change in character of the dependence of the recorded temporal parameters of switching on the radiation energy takes place. The threshold energy of radiation is determined by the thermodynamic parameters of the cathode material. Based on the experimental data, an assumption is proposed: under the action of a laser radiation pulse in the interelectrode space, glow discharge is initially ignited in the the electrode erosion products, which then as a result of the development of ionization-overheating instability, undergoes a contraction of the current channel and switches to an arc discharge. |
doi_str_mv | 10.1134/S0018151X17020018 |
format | article |
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Based on the experimental data, an assumption is proposed: under the action of a laser radiation pulse in the interelectrode space, glow discharge is initially ignited in the the electrode erosion products, which then as a result of the development of ionization-overheating instability, undergoes a contraction of the current channel and switches to an arc discharge.</description><identifier>ISSN: 0018-151X</identifier><identifier>EISSN: 1608-3156</identifier><identifier>DOI: 10.1134/S0018151X17020018</identifier><language>eng</language><publisher>Moscow: Pleiades Publishing</publisher><subject>Atoms and Molecules in Strong Fields ; Classical and Continuum Physics ; Commutation ; Delay time ; Electric arcs ; Electric sparks ; Electrode materials ; Glow discharges ; Industrial Chemistry/Chemical Engineering ; Laser Matter Interaction ; Laser plasmas ; Lasers ; Materials Science ; Overheating ; Parameters ; Physical Chemistry ; Physics ; Physics and Astronomy ; Plasma ; Plasma Investigations ; Switches ; Switching</subject><ispartof>High temperature, 2017-03, Vol.55 (2), p.191-198</ispartof><rights>Pleiades Publishing, Ltd. 2017</rights><rights>Copyright Springer Science & Business Media 2017</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c316t-434e3f590ad3096efefad0c72178e59576d46b8bbd7b51e8b7951244a43a7bd43</citedby><cites>FETCH-LOGICAL-c316t-434e3f590ad3096efefad0c72178e59576d46b8bbd7b51e8b7951244a43a7bd43</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Asyunin, V. 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The threshold energy of radiation is determined by the thermodynamic parameters of the cathode material. Based on the experimental data, an assumption is proposed: under the action of a laser radiation pulse in the interelectrode space, glow discharge is initially ignited in the the electrode erosion products, which then as a result of the development of ionization-overheating instability, undergoes a contraction of the current channel and switches to an arc discharge.</description><subject>Atoms and Molecules in Strong Fields</subject><subject>Classical and Continuum Physics</subject><subject>Commutation</subject><subject>Delay time</subject><subject>Electric arcs</subject><subject>Electric sparks</subject><subject>Electrode materials</subject><subject>Glow discharges</subject><subject>Industrial Chemistry/Chemical Engineering</subject><subject>Laser Matter Interaction</subject><subject>Laser plasmas</subject><subject>Lasers</subject><subject>Materials Science</subject><subject>Overheating</subject><subject>Parameters</subject><subject>Physical Chemistry</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Plasma</subject><subject>Plasma Investigations</subject><subject>Switches</subject><subject>Switching</subject><issn>0018-151X</issn><issn>1608-3156</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNp1UMlKxEAQbUTBcfQDvDV4jnalt-QogxsMeHAEb6HTqcxkzGZ3R5m_NyEeBPFUy1uKeoRcArsG4OLmhTFIQMIbaBZP_RFZgGJJxEGqY7KYVtGEn5Iz7_eMMSljviD1Zoe0d51F72lXUts1zRBMqLp2Gn1j6pp-GjsMDd2a3tOvKuxo1Vahmkn5gZqWYo02uMpS3xv3TvvajMoRKOjYoftZnJOT0tQeL37qkrze321Wj9H6-eFpdbuOLAcVIsEF8lKmzBScpQpLLE3BrI5BJyhTqVUhVJ7keaFzCZjkOpUQC2EENzovBF-Sq9l3fOxjQB-yfTe4djyZQZLKRCnGJhbMLOs67x2WWe-qxrhDBiybQs3-hDpq4lnjR267RffL-V_RNyhpecU</recordid><startdate>20170301</startdate><enddate>20170301</enddate><creator>Asyunin, V. 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I.</creatorcontrib><creatorcontrib>Davydov, S. G.</creatorcontrib><creatorcontrib>Dolgov, A. N.</creatorcontrib><creatorcontrib>Kozlovskaya, T. I.</creatorcontrib><creatorcontrib>Revazov, V. O.</creatorcontrib><creatorcontrib>Seleznev, V. P.</creatorcontrib><creatorcontrib>Yakubov, R. H.</creatorcontrib><collection>CrossRef</collection><jtitle>High temperature</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Asyunin, V. I.</au><au>Davydov, S. G.</au><au>Dolgov, A. N.</au><au>Kozlovskaya, T. I.</au><au>Revazov, V. O.</au><au>Seleznev, V. P.</au><au>Yakubov, R. H.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The process of commutation of small vacuum gaps with initiation by an electric spark plasma and laser plasma</atitle><jtitle>High temperature</jtitle><stitle>High Temp</stitle><date>2017-03-01</date><risdate>2017</risdate><volume>55</volume><issue>2</issue><spage>191</spage><epage>198</epage><pages>191-198</pages><issn>0018-151X</issn><eissn>1608-3156</eissn><abstract>For a vacuum spark gap with initiation by an electric spark plasma, the limited possibilities of controlling the delay time of switching by varying the energy of the auxiliary discharge are demonstrated. For a vacuum spark gap with initiation by a laser plasma, the threshold value of the radiation energy is detected at which the change in character of the dependence of the recorded temporal parameters of switching on the radiation energy takes place. The threshold energy of radiation is determined by the thermodynamic parameters of the cathode material. Based on the experimental data, an assumption is proposed: under the action of a laser radiation pulse in the interelectrode space, glow discharge is initially ignited in the the electrode erosion products, which then as a result of the development of ionization-overheating instability, undergoes a contraction of the current channel and switches to an arc discharge.</abstract><cop>Moscow</cop><pub>Pleiades Publishing</pub><doi>10.1134/S0018151X17020018</doi><tpages>8</tpages></addata></record> |
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subjects | Atoms and Molecules in Strong Fields Classical and Continuum Physics Commutation Delay time Electric arcs Electric sparks Electrode materials Glow discharges Industrial Chemistry/Chemical Engineering Laser Matter Interaction Laser plasmas Lasers Materials Science Overheating Parameters Physical Chemistry Physics Physics and Astronomy Plasma Plasma Investigations Switches Switching |
title | The process of commutation of small vacuum gaps with initiation by an electric spark plasma and laser plasma |
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