Assessment of the beam path deflection for a vertically installed microwave interferometer in SUNIST
Microwave interferometry has been widely employed to provide reliable line averaged electron density measurement on plasma devices. For a vertically installed interferometer on a tokamak, the refraction problem, which distorts the beam path and aggravates power loss at the receiving antenna, may bec...
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Veröffentlicht in: | Review of scientific instruments 2016-08, Vol.87 (8), p.083501-083501 |
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description | Microwave interferometry has been widely employed to provide reliable line averaged electron density measurement on plasma devices. For a vertically installed interferometer on a tokamak, the refraction problem, which distorts the beam path and aggravates power loss at the receiving antenna, may become significant if taking the cross section shape into account. Increasing the frequency of the probing microwave can alleviate the distortion, but at the expense of losing the density resolution. To seek for an optimized frequency, previous calculations are mainly based on the cylindrical column geometry which grossly underestimates the deflection of the beam path induced by the plasma shape, and empirical suggestions indicating n
e0/nc
= 1/2 ∼ 1/3 may not always be the appropriate option. Here a single ray tracing method is applied to estimate the final horizontal deviation at the receiving antenna, which is supposed to represent the level of power loss. The calculation is carried out under the real tokamak geometry in Sino-UNIted Spherical Tokamak (SUNIST) with the cross section parameters obtained from the equilibrium reconstruction, and the result indicates that for a target density of 1.2 × 1019 m−3, a frequency of at least 100 GHz is desirable to reduce the power loss to an acceptable level. This would be helpful for the design of a vertically installed interferometer on SUNIST. |
doi_str_mv | 10.1063/1.4959979 |
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e0/nc
= 1/2 ∼ 1/3 may not always be the appropriate option. Here a single ray tracing method is applied to estimate the final horizontal deviation at the receiving antenna, which is supposed to represent the level of power loss. The calculation is carried out under the real tokamak geometry in Sino-UNIted Spherical Tokamak (SUNIST) with the cross section parameters obtained from the equilibrium reconstruction, and the result indicates that for a target density of 1.2 × 1019 m−3, a frequency of at least 100 GHz is desirable to reduce the power loss to an acceptable level. This would be helpful for the design of a vertically installed interferometer on SUNIST.</description><identifier>ISSN: 0034-6748</identifier><identifier>EISSN: 1089-7623</identifier><identifier>DOI: 10.1063/1.4959979</identifier><identifier>PMID: 27587117</identifier><identifier>CODEN: RSINAK</identifier><language>eng</language><publisher>United States: American Institute of Physics</publisher><subject>ANTENNAS ; BEAMS ; CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY ; CROSS SECTIONS ; CYLINDRICAL CONFIGURATION ; Deflection ; DENSITY ; ELECTRON DENSITY ; Electron density measurement ; ELECTRONS ; GEOMETRY ; GHZ RANGE 01-100 ; INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY ; INTERFEROMETERS ; INTERFEROMETRY ; Mathematical analysis ; MICROWAVE RADIATION ; Plasma ; Power loss ; POWER LOSSES ; Ray tracing ; SPHERICAL CONFIGURATION ; SUNIST SPHEROMAK ; Tokamak devices</subject><ispartof>Review of scientific instruments, 2016-08, Vol.87 (8), p.083501-083501</ispartof><rights>Author(s)</rights><rights>2016 Author(s). Published by AIP Publishing.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c481t-890a7a14e35502224e85bd1ca7f5ce0316a52a06f41a9e9484d7fe62ec732a9d3</citedby><cites>FETCH-LOGICAL-c481t-890a7a14e35502224e85bd1ca7f5ce0316a52a06f41a9e9484d7fe62ec732a9d3</cites><orcidid>0000-0002-7718-7403</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/rsi/article-lookup/doi/10.1063/1.4959979$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>230,314,780,784,794,885,4512,27924,27925,76384</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/27587117$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink><backlink>$$Uhttps://www.osti.gov/biblio/22597757$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Zhong, H.</creatorcontrib><creatorcontrib>Ling, B. L.</creatorcontrib><creatorcontrib>Tan, Y.</creatorcontrib><creatorcontrib>Gao, Z.</creatorcontrib><title>Assessment of the beam path deflection for a vertically installed microwave interferometer in SUNIST</title><title>Review of scientific instruments</title><addtitle>Rev Sci Instrum</addtitle><description>Microwave interferometry has been widely employed to provide reliable line averaged electron density measurement on plasma devices. For a vertically installed interferometer on a tokamak, the refraction problem, which distorts the beam path and aggravates power loss at the receiving antenna, may become significant if taking the cross section shape into account. Increasing the frequency of the probing microwave can alleviate the distortion, but at the expense of losing the density resolution. To seek for an optimized frequency, previous calculations are mainly based on the cylindrical column geometry which grossly underestimates the deflection of the beam path induced by the plasma shape, and empirical suggestions indicating n
e0/nc
= 1/2 ∼ 1/3 may not always be the appropriate option. Here a single ray tracing method is applied to estimate the final horizontal deviation at the receiving antenna, which is supposed to represent the level of power loss. The calculation is carried out under the real tokamak geometry in Sino-UNIted Spherical Tokamak (SUNIST) with the cross section parameters obtained from the equilibrium reconstruction, and the result indicates that for a target density of 1.2 × 1019 m−3, a frequency of at least 100 GHz is desirable to reduce the power loss to an acceptable level. This would be helpful for the design of a vertically installed interferometer on SUNIST.</description><subject>ANTENNAS</subject><subject>BEAMS</subject><subject>CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY</subject><subject>CROSS SECTIONS</subject><subject>CYLINDRICAL CONFIGURATION</subject><subject>Deflection</subject><subject>DENSITY</subject><subject>ELECTRON DENSITY</subject><subject>Electron density measurement</subject><subject>ELECTRONS</subject><subject>GEOMETRY</subject><subject>GHZ RANGE 01-100</subject><subject>INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY</subject><subject>INTERFEROMETERS</subject><subject>INTERFEROMETRY</subject><subject>Mathematical analysis</subject><subject>MICROWAVE RADIATION</subject><subject>Plasma</subject><subject>Power loss</subject><subject>POWER LOSSES</subject><subject>Ray tracing</subject><subject>SPHERICAL CONFIGURATION</subject><subject>SUNIST SPHEROMAK</subject><subject>Tokamak devices</subject><issn>0034-6748</issn><issn>1089-7623</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNp90U1rGzEQBmBRGho37aF_oAh6aQqbarT6WB1DaNpASA9JzkLWjvCG3ZUryS7595Wxm5wSXfTBw4tmhpBPwM6AqfY7nAkjjdHmDVkA60yjFW_fkgVjrWiUFt0xeZ_zA6tLArwjx1zLTgPoBenPc8acJ5wLjYGWFdIluomuXVnRHsOIvgxxpiEm6ugWUxm8G8dHOsy51AP2dBp8in_dFutbwRQwxQnroV7p7f3N1e3dB3IU3Jjx42E_IfeXP-4ufjXXv39eXZxfN150UJrOMKcdCGylZJxzgZ1c9uCdDtIja0E5yR1TQYAzaEQneh1QcfS65c707Qn5ss-NuQw2-6GgX_k4z7UIy7k0Wktd1de9Wqf4Z4O52GnIHsfRzRg32UIHSnFjuHoOfKIPcZPmWoPlwEEzJVtW1ele1T7knDDYdRomlx4tMLsbkAV7GFC1nw-Jm-WE_ZP8P5EKvu3B7vtu1_tX017E25ieoV33of0H6omlrQ</recordid><startdate>20160801</startdate><enddate>20160801</enddate><creator>Zhong, H.</creator><creator>Ling, B. L.</creator><creator>Tan, Y.</creator><creator>Gao, Z.</creator><general>American Institute of Physics</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>7X8</scope><scope>OTOTI</scope><orcidid>https://orcid.org/0000-0002-7718-7403</orcidid></search><sort><creationdate>20160801</creationdate><title>Assessment of the beam path deflection for a vertically installed microwave interferometer in SUNIST</title><author>Zhong, H. ; Ling, B. L. ; Tan, Y. ; Gao, Z.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c481t-890a7a14e35502224e85bd1ca7f5ce0316a52a06f41a9e9484d7fe62ec732a9d3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>ANTENNAS</topic><topic>BEAMS</topic><topic>CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY</topic><topic>CROSS SECTIONS</topic><topic>CYLINDRICAL CONFIGURATION</topic><topic>Deflection</topic><topic>DENSITY</topic><topic>ELECTRON DENSITY</topic><topic>Electron density measurement</topic><topic>ELECTRONS</topic><topic>GEOMETRY</topic><topic>GHZ RANGE 01-100</topic><topic>INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY</topic><topic>INTERFEROMETERS</topic><topic>INTERFEROMETRY</topic><topic>Mathematical analysis</topic><topic>MICROWAVE RADIATION</topic><topic>Plasma</topic><topic>Power loss</topic><topic>POWER LOSSES</topic><topic>Ray tracing</topic><topic>SPHERICAL CONFIGURATION</topic><topic>SUNIST SPHEROMAK</topic><topic>Tokamak devices</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Zhong, H.</creatorcontrib><creatorcontrib>Ling, B. L.</creatorcontrib><creatorcontrib>Tan, Y.</creatorcontrib><creatorcontrib>Gao, Z.</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><collection>OSTI.GOV</collection><jtitle>Review of scientific instruments</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Zhong, H.</au><au>Ling, B. L.</au><au>Tan, Y.</au><au>Gao, Z.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Assessment of the beam path deflection for a vertically installed microwave interferometer in SUNIST</atitle><jtitle>Review of scientific instruments</jtitle><addtitle>Rev Sci Instrum</addtitle><date>2016-08-01</date><risdate>2016</risdate><volume>87</volume><issue>8</issue><spage>083501</spage><epage>083501</epage><pages>083501-083501</pages><issn>0034-6748</issn><eissn>1089-7623</eissn><coden>RSINAK</coden><abstract>Microwave interferometry has been widely employed to provide reliable line averaged electron density measurement on plasma devices. For a vertically installed interferometer on a tokamak, the refraction problem, which distorts the beam path and aggravates power loss at the receiving antenna, may become significant if taking the cross section shape into account. Increasing the frequency of the probing microwave can alleviate the distortion, but at the expense of losing the density resolution. To seek for an optimized frequency, previous calculations are mainly based on the cylindrical column geometry which grossly underestimates the deflection of the beam path induced by the plasma shape, and empirical suggestions indicating n
e0/nc
= 1/2 ∼ 1/3 may not always be the appropriate option. Here a single ray tracing method is applied to estimate the final horizontal deviation at the receiving antenna, which is supposed to represent the level of power loss. The calculation is carried out under the real tokamak geometry in Sino-UNIted Spherical Tokamak (SUNIST) with the cross section parameters obtained from the equilibrium reconstruction, and the result indicates that for a target density of 1.2 × 1019 m−3, a frequency of at least 100 GHz is desirable to reduce the power loss to an acceptable level. This would be helpful for the design of a vertically installed interferometer on SUNIST.</abstract><cop>United States</cop><pub>American Institute of Physics</pub><pmid>27587117</pmid><doi>10.1063/1.4959979</doi><tpages>3</tpages><orcidid>https://orcid.org/0000-0002-7718-7403</orcidid></addata></record> |
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subjects | ANTENNAS BEAMS CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY CROSS SECTIONS CYLINDRICAL CONFIGURATION Deflection DENSITY ELECTRON DENSITY Electron density measurement ELECTRONS GEOMETRY GHZ RANGE 01-100 INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY INTERFEROMETERS INTERFEROMETRY Mathematical analysis MICROWAVE RADIATION Plasma Power loss POWER LOSSES Ray tracing SPHERICAL CONFIGURATION SUNIST SPHEROMAK Tokamak devices |
title | Assessment of the beam path deflection for a vertically installed microwave interferometer in SUNIST |
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