Analysis of Heat Load in a Superconducting Wiggler With a Semi-Cold UHV Beam Duct
A superconducting wiggler with a magnetic period of 6.0 cm (SW6) and a peak field of 3.2 T has been designed and fabricated in the National Synchrotron Radiation Research Center (NSRRC). The beam duct separates the electron beam from the cryogenic system of the magnet. The heat load on the beam duct...
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Veröffentlicht in: | IEEE transactions on applied superconductivity 2006-06, Vol.16 (2), p.1320-1323 |
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container_title | IEEE transactions on applied superconductivity |
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creator | Chen, H.H. Hwang, C.S. Chang, C.H. Lin, F.Y. Hsu, S.N. Chang, C.C. Hsiung, G.Y. Chen, J.R. |
description | A superconducting wiggler with a magnetic period of 6.0 cm (SW6) and a peak field of 3.2 T has been designed and fabricated in the National Synchrotron Radiation Research Center (NSRRC). The beam duct separates the electron beam from the cryogenic system of the magnet. The heat load on the beam duct should be low to stabilize the operation of the superconducting magnets. However, outgassing caused by synchrotron radiation at an electron energy of 1.5 GeV and a current of 200 mA must be reduced. Accordingly, operating the system at a higher temperature can minimize the adsorption of molecules on the beam duct. Therefore, the beam duct system and its connection by finite element analysis are designed to optimize the operating temperature of the beam duct at between 100 and 120 K. Performance of the beam duct is established to comply with specifications during the operation of magnet |
doi_str_mv | 10.1109/TASC.2006.871211 |
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The beam duct separates the electron beam from the cryogenic system of the magnet. The heat load on the beam duct should be low to stabilize the operation of the superconducting magnets. However, outgassing caused by synchrotron radiation at an electron energy of 1.5 GeV and a current of 200 mA must be reduced. Accordingly, operating the system at a higher temperature can minimize the adsorption of molecules on the beam duct. Therefore, the beam duct system and its connection by finite element analysis are designed to optimize the operating temperature of the beam duct at between 100 and 120 K. Performance of the beam duct is established to comply with specifications during the operation of magnet</description><identifier>ISSN: 1051-8223</identifier><identifier>EISSN: 1558-2515</identifier><identifier>DOI: 10.1109/TASC.2006.871211</identifier><identifier>CODEN: ITASE9</identifier><language>eng</language><publisher>New York, NY: IEEE</publisher><subject>Applied sciences ; Beams (radiation) ; Cryogenics ; Ducts ; Electrical engineering. Electrical power engineering ; Electrical power engineering ; Electromagnets ; Electron beams ; Exact sciences and technology ; Finite element methods ; Magnet cryostat ; Magnetic analysis ; Magnetic separation ; Mathematical analysis ; Operating temperature ; Power networks and lines ; semi-cold UHV beam duct ; Specifications ; Superconducting magnets ; superconducting wiggler ; Superconductivity ; Synchrotron radiation ; Temperature ; thermal interception ; Undulators ; Users connections and in door installation ; Various equipment and components</subject><ispartof>IEEE transactions on applied superconductivity, 2006-06, Vol.16 (2), p.1320-1323</ispartof><rights>2006 INIST-CNRS</rights><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. 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The beam duct separates the electron beam from the cryogenic system of the magnet. The heat load on the beam duct should be low to stabilize the operation of the superconducting magnets. However, outgassing caused by synchrotron radiation at an electron energy of 1.5 GeV and a current of 200 mA must be reduced. Accordingly, operating the system at a higher temperature can minimize the adsorption of molecules on the beam duct. Therefore, the beam duct system and its connection by finite element analysis are designed to optimize the operating temperature of the beam duct at between 100 and 120 K. Performance of the beam duct is established to comply with specifications during the operation of magnet</description><subject>Applied sciences</subject><subject>Beams (radiation)</subject><subject>Cryogenics</subject><subject>Ducts</subject><subject>Electrical engineering. Electrical power engineering</subject><subject>Electrical power engineering</subject><subject>Electromagnets</subject><subject>Electron beams</subject><subject>Exact sciences and technology</subject><subject>Finite element methods</subject><subject>Magnet cryostat</subject><subject>Magnetic analysis</subject><subject>Magnetic separation</subject><subject>Mathematical analysis</subject><subject>Operating temperature</subject><subject>Power networks and lines</subject><subject>semi-cold UHV beam duct</subject><subject>Specifications</subject><subject>Superconducting magnets</subject><subject>superconducting wiggler</subject><subject>Superconductivity</subject><subject>Synchrotron radiation</subject><subject>Temperature</subject><subject>thermal interception</subject><subject>Undulators</subject><subject>Users connections and in door installation</subject><subject>Various equipment and components</subject><issn>1051-8223</issn><issn>1558-2515</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2006</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNpdkEtLw0AUhQdRsFb3gptBEFepM5N5ZVnjo0JBpK0uwyS5qSN51Jlk0X9vQgoFV-fC_c6BcxC6pmRGKYke1vNVPGOEyJlWlFF6giZUCB0wQcVpfxNBA81YeI4uvP8hhHLNxQR9zGtT7r31uCnwAkyLl43Jsa2xwatuBy5r6rzLWltv8ZfdbktwvbbfwxsqG8RNmePN4hM_gqnwU09eorPClB6uDjpFm5fndbwIlu-vb_F8GWShYG3AFdG5YUIWoA1PDZNFSiElOpJ5DmEuIsqM6gvRNExBKc6lkkJkIUlpxHMZTtH9mLtzzW8Hvk0q6zMoS1ND0_kkolxyppjoydt_5E_Tub73ADFGFNe6h8gIZa7x3kGR7JytjNsnlCTDwsmwcDIsnIwL95a7Q67xmSkLZ-rM-qNPRTxScuBuRs4CwPEteUgiHv4B_hyA5Q</recordid><startdate>20060601</startdate><enddate>20060601</enddate><creator>Chen, H.H.</creator><creator>Hwang, C.S.</creator><creator>Chang, C.H.</creator><creator>Lin, F.Y.</creator><creator>Hsu, S.N.</creator><creator>Chang, C.C.</creator><creator>Hsiung, G.Y.</creator><creator>Chen, J.R.</creator><general>IEEE</general><general>Institute of Electrical and Electronics Engineers</general><general>The Institute of Electrical and Electronics Engineers, Inc. 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The beam duct separates the electron beam from the cryogenic system of the magnet. The heat load on the beam duct should be low to stabilize the operation of the superconducting magnets. However, outgassing caused by synchrotron radiation at an electron energy of 1.5 GeV and a current of 200 mA must be reduced. Accordingly, operating the system at a higher temperature can minimize the adsorption of molecules on the beam duct. Therefore, the beam duct system and its connection by finite element analysis are designed to optimize the operating temperature of the beam duct at between 100 and 120 K. Performance of the beam duct is established to comply with specifications during the operation of magnet</abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/TASC.2006.871211</doi><tpages>4</tpages></addata></record> |
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subjects | Applied sciences Beams (radiation) Cryogenics Ducts Electrical engineering. Electrical power engineering Electrical power engineering Electromagnets Electron beams Exact sciences and technology Finite element methods Magnet cryostat Magnetic analysis Magnetic separation Mathematical analysis Operating temperature Power networks and lines semi-cold UHV beam duct Specifications Superconducting magnets superconducting wiggler Superconductivity Synchrotron radiation Temperature thermal interception Undulators Users connections and in door installation Various equipment and components |
title | Analysis of Heat Load in a Superconducting Wiggler With a Semi-Cold UHV Beam Duct |
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