Loading…

Experimental study on the ionization of argon behind reflected shock waves

The electron temperature and density along with the ion temperature in argon gas behind reflected shock waves were measured by laser light scattering, while the spectroscopic temperature was measured from the ArI line emissions. The values of these three temperatures are different from each other fo...

Full description

Saved in:
Bibliographic Details
Published in:Japanese Journal of Applied Physics 1983-01, Vol.22 (4), p.735-741
Main Authors: TERAO, K, HOZAKA, M, KAITOH, H
Format: Article
Language:English
Subjects:
Citations: Items that this one cites
Items that cite this one
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
cited_by cdi_FETCH-LOGICAL-c355t-7100a2e8b1042c4ae3e8100c303a69936dddbca7605cb695e8d93905816e5c903
cites cdi_FETCH-LOGICAL-c355t-7100a2e8b1042c4ae3e8100c303a69936dddbca7605cb695e8d93905816e5c903
container_end_page 741
container_issue 4
container_start_page 735
container_title Japanese Journal of Applied Physics
container_volume 22
creator TERAO, K
HOZAKA, M
KAITOH, H
description The electron temperature and density along with the ion temperature in argon gas behind reflected shock waves were measured by laser light scattering, while the spectroscopic temperature was measured from the ArI line emissions. The values of these three temperatures are different from each other for a few hundred microseconds after arrival of the reflected shock front. Both the electron and ion temperatures are much higher than the theoretical gasdynamic temperature, while the spectroscopic temperature is lower than the theoretical one. The degree of ionization is much higher than that in the equilibrium state. The stochastic character of the ArI line emissions was observed, indicating that the gas is inhomogeneous. These phenomena are explained as follows: initially, the gas behind the reflected shock wave is inhomogeneous, and an associative ionization is initiated at some points. The gas becomes homogeneous mainly through diffusion.
doi_str_mv 10.1143/jjap.22.735
format article
fullrecord <record><control><sourceid>pascalfrancis_cross</sourceid><recordid>TN_cdi_crossref_primary_10_1143_JJAP_22_735</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>9456427</sourcerecordid><originalsourceid>FETCH-LOGICAL-c355t-7100a2e8b1042c4ae3e8100c303a69936dddbca7605cb695e8d93905816e5c903</originalsourceid><addsrcrecordid>eNo9UMtOwzAQtBBIlMKJH_CBG0rwO_GxqkqhqgQHOEcbe0NSQhLF4VG-HqMiTrO7mlnNDCGXnKWcK3mz28GQCpFmUh-RGZcqSxQz-pjMGBM8UVaIU3IWwi6uRis-I5vV14Bj84bdBC0N07vf076jU4206bvmG6YItK8ojC9xKLFuOk9HrFp0E3oa6t690k_4wHBOTipoA1784Zw8366elnfJ9mF9v1xsEye1npKMMwYC85IzJZwClJjHk5NMgrFWGu996SAzTLvSWI25t9IynXOD2lkm5-T68NeNfQjRSjHEADDuC86K3xqKzWbxWAhRxBoi--rAHiA4aKsROteEf4lV2iiRyR_FLVz5</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Experimental study on the ionization of argon behind reflected shock waves</title><source>Institute of Physics IOP Science Extra</source><source>Institute of Physics:Jisc Collections:IOP Publishing Read and Publish 2024-2025 (Reading List)</source><creator>TERAO, K ; HOZAKA, M ; KAITOH, H</creator><creatorcontrib>TERAO, K ; HOZAKA, M ; KAITOH, H</creatorcontrib><description>The electron temperature and density along with the ion temperature in argon gas behind reflected shock waves were measured by laser light scattering, while the spectroscopic temperature was measured from the ArI line emissions. The values of these three temperatures are different from each other for a few hundred microseconds after arrival of the reflected shock front. Both the electron and ion temperatures are much higher than the theoretical gasdynamic temperature, while the spectroscopic temperature is lower than the theoretical one. The degree of ionization is much higher than that in the equilibrium state. The stochastic character of the ArI line emissions was observed, indicating that the gas is inhomogeneous. These phenomena are explained as follows: initially, the gas behind the reflected shock wave is inhomogeneous, and an associative ionization is initiated at some points. The gas becomes homogeneous mainly through diffusion.</description><identifier>ISSN: 0021-4922</identifier><identifier>EISSN: 1347-4065</identifier><identifier>DOI: 10.1143/jjap.22.735</identifier><identifier>CODEN: JJAPA5</identifier><language>eng</language><publisher>Tokyo: Japanese journal of applied physics</publisher><subject>Exact sciences and technology ; Physics ; Physics of gases, plasmas and electric discharges ; Physics of plasmas and electric discharges ; Plasma diagnostic techniques and instrumentation</subject><ispartof>Japanese Journal of Applied Physics, 1983-01, Vol.22 (4), p.735-741</ispartof><rights>1984 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c355t-7100a2e8b1042c4ae3e8100c303a69936dddbca7605cb695e8d93905816e5c903</citedby><cites>FETCH-LOGICAL-c355t-7100a2e8b1042c4ae3e8100c303a69936dddbca7605cb695e8d93905816e5c903</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27923,27924</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&amp;idt=9456427$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>TERAO, K</creatorcontrib><creatorcontrib>HOZAKA, M</creatorcontrib><creatorcontrib>KAITOH, H</creatorcontrib><title>Experimental study on the ionization of argon behind reflected shock waves</title><title>Japanese Journal of Applied Physics</title><description>The electron temperature and density along with the ion temperature in argon gas behind reflected shock waves were measured by laser light scattering, while the spectroscopic temperature was measured from the ArI line emissions. The values of these three temperatures are different from each other for a few hundred microseconds after arrival of the reflected shock front. Both the electron and ion temperatures are much higher than the theoretical gasdynamic temperature, while the spectroscopic temperature is lower than the theoretical one. The degree of ionization is much higher than that in the equilibrium state. The stochastic character of the ArI line emissions was observed, indicating that the gas is inhomogeneous. These phenomena are explained as follows: initially, the gas behind the reflected shock wave is inhomogeneous, and an associative ionization is initiated at some points. The gas becomes homogeneous mainly through diffusion.</description><subject>Exact sciences and technology</subject><subject>Physics</subject><subject>Physics of gases, plasmas and electric discharges</subject><subject>Physics of plasmas and electric discharges</subject><subject>Plasma diagnostic techniques and instrumentation</subject><issn>0021-4922</issn><issn>1347-4065</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1983</creationdate><recordtype>article</recordtype><recordid>eNo9UMtOwzAQtBBIlMKJH_CBG0rwO_GxqkqhqgQHOEcbe0NSQhLF4VG-HqMiTrO7mlnNDCGXnKWcK3mz28GQCpFmUh-RGZcqSxQz-pjMGBM8UVaIU3IWwi6uRis-I5vV14Bj84bdBC0N07vf076jU4206bvmG6YItK8ojC9xKLFuOk9HrFp0E3oa6t690k_4wHBOTipoA1784Zw8366elnfJ9mF9v1xsEye1npKMMwYC85IzJZwClJjHk5NMgrFWGu996SAzTLvSWI25t9IynXOD2lkm5-T68NeNfQjRSjHEADDuC86K3xqKzWbxWAhRxBoi--rAHiA4aKsROteEf4lV2iiRyR_FLVz5</recordid><startdate>19830101</startdate><enddate>19830101</enddate><creator>TERAO, K</creator><creator>HOZAKA, M</creator><creator>KAITOH, H</creator><general>Japanese journal of applied physics</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>19830101</creationdate><title>Experimental study on the ionization of argon behind reflected shock waves</title><author>TERAO, K ; HOZAKA, M ; KAITOH, H</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c355t-7100a2e8b1042c4ae3e8100c303a69936dddbca7605cb695e8d93905816e5c903</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1983</creationdate><topic>Exact sciences and technology</topic><topic>Physics</topic><topic>Physics of gases, plasmas and electric discharges</topic><topic>Physics of plasmas and electric discharges</topic><topic>Plasma diagnostic techniques and instrumentation</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>TERAO, K</creatorcontrib><creatorcontrib>HOZAKA, M</creatorcontrib><creatorcontrib>KAITOH, H</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><jtitle>Japanese Journal of Applied Physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>TERAO, K</au><au>HOZAKA, M</au><au>KAITOH, H</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Experimental study on the ionization of argon behind reflected shock waves</atitle><jtitle>Japanese Journal of Applied Physics</jtitle><date>1983-01-01</date><risdate>1983</risdate><volume>22</volume><issue>4</issue><spage>735</spage><epage>741</epage><pages>735-741</pages><issn>0021-4922</issn><eissn>1347-4065</eissn><coden>JJAPA5</coden><abstract>The electron temperature and density along with the ion temperature in argon gas behind reflected shock waves were measured by laser light scattering, while the spectroscopic temperature was measured from the ArI line emissions. The values of these three temperatures are different from each other for a few hundred microseconds after arrival of the reflected shock front. Both the electron and ion temperatures are much higher than the theoretical gasdynamic temperature, while the spectroscopic temperature is lower than the theoretical one. The degree of ionization is much higher than that in the equilibrium state. The stochastic character of the ArI line emissions was observed, indicating that the gas is inhomogeneous. These phenomena are explained as follows: initially, the gas behind the reflected shock wave is inhomogeneous, and an associative ionization is initiated at some points. The gas becomes homogeneous mainly through diffusion.</abstract><cop>Tokyo</cop><pub>Japanese journal of applied physics</pub><doi>10.1143/jjap.22.735</doi><tpages>7</tpages></addata></record>
fulltext fulltext
identifier ISSN: 0021-4922
ispartof Japanese Journal of Applied Physics, 1983-01, Vol.22 (4), p.735-741
issn 0021-4922
1347-4065
language eng
recordid cdi_crossref_primary_10_1143_JJAP_22_735
source Institute of Physics IOP Science Extra; Institute of Physics:Jisc Collections:IOP Publishing Read and Publish 2024-2025 (Reading List)
subjects Exact sciences and technology
Physics
Physics of gases, plasmas and electric discharges
Physics of plasmas and electric discharges
Plasma diagnostic techniques and instrumentation
title Experimental study on the ionization of argon behind reflected shock waves
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-08T23%3A50%3A50IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-pascalfrancis_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Experimental%20study%20on%20the%20ionization%20of%20argon%20behind%20reflected%20shock%20waves&rft.jtitle=Japanese%20Journal%20of%20Applied%20Physics&rft.au=TERAO,%20K&rft.date=1983-01-01&rft.volume=22&rft.issue=4&rft.spage=735&rft.epage=741&rft.pages=735-741&rft.issn=0021-4922&rft.eissn=1347-4065&rft.coden=JJAPA5&rft_id=info:doi/10.1143/jjap.22.735&rft_dat=%3Cpascalfrancis_cross%3E9456427%3C/pascalfrancis_cross%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c355t-7100a2e8b1042c4ae3e8100c303a69936dddbca7605cb695e8d93905816e5c903%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true