High-power gyrotron development at Forschungszentrum Karlsruhe for fusion applications

In the first part of this paper, the status of the 140-GHz continuously operated gyrotrons with an output power of 1 MW for the stellarator Wendelstein 7-X will be described. With the first series tube, an output power of 1000 kW has been achieved in short pulse operation (milliseconds) with an elec...

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Veröffentlicht in:IEEE transactions on plasma science 2006-04, Vol.34 (2), p.173-186
Hauptverfasser: Dammertz, G., Alberti, S., Arnold, A., Bariou, D., Brand, P., Braune, H., Erckmann, V., Dumbrajs, O., Gantenbein, G., Giguet, E., Heidinger, R., Hogge, J.-P., Illy, S., Jin, J., Kasparek, W., Koppenburg, K., Laqua, H.P., Legrand, F., Leonhardt, W., Lievin, C., Michel, G., Neffe, G., Piosczyk, B., Prinz, O., Rzesnicki, T., Schmid, M., Thumm, M., Minh Quang Tran, Yang, X., Yovchev, I.
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container_issue 2
container_start_page 173
container_title IEEE transactions on plasma science
container_volume 34
creator Dammertz, G.
Alberti, S.
Arnold, A.
Bariou, D.
Brand, P.
Braune, H.
Erckmann, V.
Dumbrajs, O.
Gantenbein, G.
Giguet, E.
Heidinger, R.
Hogge, J.-P.
Illy, S.
Jin, J.
Kasparek, W.
Koppenburg, K.
Laqua, H.P.
Legrand, F.
Leonhardt, W.
Lievin, C.
Michel, G.
Neffe, G.
Piosczyk, B.
Prinz, O.
Rzesnicki, T.
Schmid, M.
Thumm, M.
Minh Quang Tran
Yang, X.
Yovchev, I.
description In the first part of this paper, the status of the 140-GHz continuously operated gyrotrons with an output power of 1 MW for the stellarator Wendelstein 7-X will be described. With the first series tube, an output power of 1000 kW has been achieved in short pulse operation (milliseconds) with an electron beam current of 40 A, and of 1150 kW at 50 A. With a pulse length of 3 min limited by the available high-voltage (HV) power supply, an output power of 920 kW at an electron beam current of about 40 A with an efficiency of 45% and a mode purity of 97.5% has been obtained. At a reduced beam current of 29 A, an output power of 570 kW was measured with a pulse length of 1893 s without significant increase in tube pressure. The energy content of this pulse is almost 1.1 GJ. For the next fusion plasma device, International Thermonuclear Experimental Reactor (ITER), gyrotrons with a higher output power of about 2 MW are desirable. In short-pulse experiments, the feasibility of the fabrication of coaxial cavity gyrotrons with an output power up to 2-MW, continuous wave (CW), has been demonstrated, and the information necessary for a technical design has been obtained. The development of a long-pulse 2-MW coaxial cavity gyrotron started within a European cooperation. In parallel to the design and fabrication of an industrial prototype gyrotron, a short-pulse preprototype gyrotron has been operated to verify the design of critical components. An output power of 1.2 MW with an efficiency of 20% has been achieved. The development of frequency tunable gyrotrons operating in the range from 105 to 140 GHz for stabilization of current driven plasma instabilities in fusion plasma devices (neoclassical tearing modes) is another task in the development of gyrotrons at the Forschungszentrum Karlsruhe.
doi_str_mv 10.1109/TPS.2006.872176
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With the first series tube, an output power of 1000 kW has been achieved in short pulse operation (milliseconds) with an electron beam current of 40 A, and of 1150 kW at 50 A. With a pulse length of 3 min limited by the available high-voltage (HV) power supply, an output power of 920 kW at an electron beam current of about 40 A with an efficiency of 45% and a mode purity of 97.5% has been obtained. At a reduced beam current of 29 A, an output power of 570 kW was measured with a pulse length of 1893 s without significant increase in tube pressure. The energy content of this pulse is almost 1.1 GJ. For the next fusion plasma device, International Thermonuclear Experimental Reactor (ITER), gyrotrons with a higher output power of about 2 MW are desirable. In short-pulse experiments, the feasibility of the fabrication of coaxial cavity gyrotrons with an output power up to 2-MW, continuous wave (CW), has been demonstrated, and the information necessary for a technical design has been obtained. The development of a long-pulse 2-MW coaxial cavity gyrotron started within a European cooperation. In parallel to the design and fabrication of an industrial prototype gyrotron, a short-pulse preprototype gyrotron has been operated to verify the design of critical components. An output power of 1.2 MW with an efficiency of 20% has been achieved. The development of frequency tunable gyrotrons operating in the range from 105 to 140 GHz for stabilization of current driven plasma instabilities in fusion plasma devices (neoclassical tearing modes) is another task in the development of gyrotrons at the Forschungszentrum Karlsruhe.</description><identifier>ISSN: 0093-3813</identifier><identifier>EISSN: 1939-9375</identifier><identifier>DOI: 10.1109/TPS.2006.872176</identifier><identifier>CODEN: ITPSBD</identifier><language>eng</language><publisher>New York, NY: IEEE</publisher><subject>Applied sciences ; Coaxial components ; Coaxial gyrotron ; Devices ; diamond window ; Electricity generation ; Electron beams ; Electron tubes ; Electronic tubes, masers ; Electronics ; Electrons ; Exact sciences and technology ; Fabrication ; frequency tuning ; Fusion ; gyrotron ; Gyrotrons ; high-power microwaves ; Holes ; Instability ; Magnetic confinement and equilibrium ; Particle beam measurements ; Physics ; Physics of gases, plasmas and electric discharges ; Physics of plasmas and electric discharges ; Plasma ; Plasma devices ; Plasma heating (beam injection, radio-frequency and microwave, ohmic, icr, ecr and current drive heating) ; Plasma production and heating ; Power generation ; Pulse measurements ; Pulsed power supplies ; quasi-optical mode converter ; Short pulses ; single-stage depressed collector ; Stabilization ; Stellarators, torsatrons, heliacs, bumpy tori, and other toroidal confinement devices ; step tunability ; stray radiation ; Tokamaks ; Tubes</subject><ispartof>IEEE transactions on plasma science, 2006-04, Vol.34 (2), p.173-186</ispartof><rights>2006 INIST-CNRS</rights><rights>Copyright Institute of Electrical and Electronics Engineers, Inc. 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With the first series tube, an output power of 1000 kW has been achieved in short pulse operation (milliseconds) with an electron beam current of 40 A, and of 1150 kW at 50 A. With a pulse length of 3 min limited by the available high-voltage (HV) power supply, an output power of 920 kW at an electron beam current of about 40 A with an efficiency of 45% and a mode purity of 97.5% has been obtained. At a reduced beam current of 29 A, an output power of 570 kW was measured with a pulse length of 1893 s without significant increase in tube pressure. The energy content of this pulse is almost 1.1 GJ. For the next fusion plasma device, International Thermonuclear Experimental Reactor (ITER), gyrotrons with a higher output power of about 2 MW are desirable. In short-pulse experiments, the feasibility of the fabrication of coaxial cavity gyrotrons with an output power up to 2-MW, continuous wave (CW), has been demonstrated, and the information necessary for a technical design has been obtained. The development of a long-pulse 2-MW coaxial cavity gyrotron started within a European cooperation. In parallel to the design and fabrication of an industrial prototype gyrotron, a short-pulse preprototype gyrotron has been operated to verify the design of critical components. An output power of 1.2 MW with an efficiency of 20% has been achieved. The development of frequency tunable gyrotrons operating in the range from 105 to 140 GHz for stabilization of current driven plasma instabilities in fusion plasma devices (neoclassical tearing modes) is another task in the development of gyrotrons at the Forschungszentrum Karlsruhe.</description><subject>Applied sciences</subject><subject>Coaxial components</subject><subject>Coaxial gyrotron</subject><subject>Devices</subject><subject>diamond window</subject><subject>Electricity generation</subject><subject>Electron beams</subject><subject>Electron tubes</subject><subject>Electronic tubes, masers</subject><subject>Electronics</subject><subject>Electrons</subject><subject>Exact sciences and technology</subject><subject>Fabrication</subject><subject>frequency tuning</subject><subject>Fusion</subject><subject>gyrotron</subject><subject>Gyrotrons</subject><subject>high-power microwaves</subject><subject>Holes</subject><subject>Instability</subject><subject>Magnetic confinement and equilibrium</subject><subject>Particle beam measurements</subject><subject>Physics</subject><subject>Physics of gases, plasmas and electric discharges</subject><subject>Physics of plasmas and electric discharges</subject><subject>Plasma</subject><subject>Plasma devices</subject><subject>Plasma heating (beam injection, radio-frequency and microwave, ohmic, icr, ecr and current drive heating)</subject><subject>Plasma production and heating</subject><subject>Power generation</subject><subject>Pulse measurements</subject><subject>Pulsed power supplies</subject><subject>quasi-optical mode converter</subject><subject>Short pulses</subject><subject>single-stage depressed collector</subject><subject>Stabilization</subject><subject>Stellarators, torsatrons, heliacs, bumpy tori, and other toroidal confinement devices</subject><subject>step tunability</subject><subject>stray radiation</subject><subject>Tokamaks</subject><subject>Tubes</subject><issn>0093-3813</issn><issn>1939-9375</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2006</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNp9kcFLwzAUxoMoOKdnD16KoJ66JXlrkh5lOCcOFJxeQ9omW0fX1KRV5l9vxgYDD57e473f98F7H0KXBA8Iwelw_vo2oBizgeCUcHaEeiSFNE6BJ8eoh3EKMQgCp-jM-xXGZJRg2kMf03KxjBv7rV202DjbOltHhf7SlW3Wum4j1UYT63y-7OqF_wkT162jZ-Uq77qljox1kel8GVSqaaoyV23o_Tk6Mary-mJf--h98jAfT-PZy-PT-H4W5yPK2zgzORimmCLGaGAkK7hhIlUjxmmWYAGEKcEMQFZQkmiasaJIKKNKcM2AptBHdzvfxtnPTvtWrkuf66pStbadl0KEHwRjEsjbf0kqwks4HgXw-g-4sp2rwxWSpAnhAIIGaLiDcme9d9rIxpVr5TaSYLmNQ4Y45DYOuYsjKG72tsrnqjJO1XnpDzLOKWAQgbvacaXW-rBmlFCRwC-jkpO_</recordid><startdate>20060401</startdate><enddate>20060401</enddate><creator>Dammertz, G.</creator><creator>Alberti, S.</creator><creator>Arnold, A.</creator><creator>Bariou, D.</creator><creator>Brand, P.</creator><creator>Braune, H.</creator><creator>Erckmann, V.</creator><creator>Dumbrajs, O.</creator><creator>Gantenbein, G.</creator><creator>Giguet, E.</creator><creator>Heidinger, R.</creator><creator>Hogge, J.-P.</creator><creator>Illy, S.</creator><creator>Jin, J.</creator><creator>Kasparek, W.</creator><creator>Koppenburg, K.</creator><creator>Laqua, H.P.</creator><creator>Legrand, F.</creator><creator>Leonhardt, W.</creator><creator>Lievin, C.</creator><creator>Michel, G.</creator><creator>Neffe, G.</creator><creator>Piosczyk, B.</creator><creator>Prinz, O.</creator><creator>Rzesnicki, T.</creator><creator>Schmid, M.</creator><creator>Thumm, M.</creator><creator>Minh Quang Tran</creator><creator>Yang, X.</creator><creator>Yovchev, I.</creator><general>IEEE</general><general>Institute of Electrical and Electronics Engineers</general><general>The Institute of Electrical and Electronics Engineers, Inc. (IEEE)</general><scope>97E</scope><scope>RIA</scope><scope>RIE</scope><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope><scope>F28</scope><scope>FR3</scope></search><sort><creationdate>20060401</creationdate><title>High-power gyrotron development at Forschungszentrum Karlsruhe for fusion applications</title><author>Dammertz, G. ; Alberti, S. ; Arnold, A. ; Bariou, D. ; Brand, P. ; Braune, H. ; Erckmann, V. ; Dumbrajs, O. ; Gantenbein, G. ; Giguet, E. ; Heidinger, R. ; Hogge, J.-P. ; Illy, S. ; Jin, J. ; Kasparek, W. ; Koppenburg, K. ; Laqua, H.P. ; Legrand, F. ; Leonhardt, W. ; Lievin, C. ; Michel, G. ; Neffe, G. ; Piosczyk, B. ; Prinz, O. ; Rzesnicki, T. ; Schmid, M. ; Thumm, M. ; Minh Quang Tran ; Yang, X. ; Yovchev, I.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c427t-bfc3f6a6a1ffe361bd7f689a4672b508316a86f33bd215e2b6dd5262a87e63293</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2006</creationdate><topic>Applied sciences</topic><topic>Coaxial components</topic><topic>Coaxial gyrotron</topic><topic>Devices</topic><topic>diamond window</topic><topic>Electricity generation</topic><topic>Electron beams</topic><topic>Electron tubes</topic><topic>Electronic tubes, masers</topic><topic>Electronics</topic><topic>Electrons</topic><topic>Exact sciences and technology</topic><topic>Fabrication</topic><topic>frequency tuning</topic><topic>Fusion</topic><topic>gyrotron</topic><topic>Gyrotrons</topic><topic>high-power microwaves</topic><topic>Holes</topic><topic>Instability</topic><topic>Magnetic confinement and equilibrium</topic><topic>Particle beam measurements</topic><topic>Physics</topic><topic>Physics of gases, plasmas and electric discharges</topic><topic>Physics of plasmas and electric discharges</topic><topic>Plasma</topic><topic>Plasma devices</topic><topic>Plasma heating (beam injection, radio-frequency and microwave, ohmic, icr, ecr and current drive heating)</topic><topic>Plasma production and heating</topic><topic>Power generation</topic><topic>Pulse measurements</topic><topic>Pulsed power supplies</topic><topic>quasi-optical mode converter</topic><topic>Short pulses</topic><topic>single-stage depressed collector</topic><topic>Stabilization</topic><topic>Stellarators, torsatrons, heliacs, bumpy tori, and other toroidal confinement devices</topic><topic>step tunability</topic><topic>stray radiation</topic><topic>Tokamaks</topic><topic>Tubes</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Dammertz, G.</creatorcontrib><creatorcontrib>Alberti, S.</creatorcontrib><creatorcontrib>Arnold, A.</creatorcontrib><creatorcontrib>Bariou, D.</creatorcontrib><creatorcontrib>Brand, P.</creatorcontrib><creatorcontrib>Braune, H.</creatorcontrib><creatorcontrib>Erckmann, V.</creatorcontrib><creatorcontrib>Dumbrajs, O.</creatorcontrib><creatorcontrib>Gantenbein, G.</creatorcontrib><creatorcontrib>Giguet, E.</creatorcontrib><creatorcontrib>Heidinger, R.</creatorcontrib><creatorcontrib>Hogge, J.-P.</creatorcontrib><creatorcontrib>Illy, S.</creatorcontrib><creatorcontrib>Jin, J.</creatorcontrib><creatorcontrib>Kasparek, W.</creatorcontrib><creatorcontrib>Koppenburg, K.</creatorcontrib><creatorcontrib>Laqua, H.P.</creatorcontrib><creatorcontrib>Legrand, F.</creatorcontrib><creatorcontrib>Leonhardt, W.</creatorcontrib><creatorcontrib>Lievin, C.</creatorcontrib><creatorcontrib>Michel, G.</creatorcontrib><creatorcontrib>Neffe, G.</creatorcontrib><creatorcontrib>Piosczyk, B.</creatorcontrib><creatorcontrib>Prinz, O.</creatorcontrib><creatorcontrib>Rzesnicki, T.</creatorcontrib><creatorcontrib>Schmid, M.</creatorcontrib><creatorcontrib>Thumm, M.</creatorcontrib><creatorcontrib>Minh Quang Tran</creatorcontrib><creatorcontrib>Yang, X.</creatorcontrib><creatorcontrib>Yovchev, I.</creatorcontrib><collection>IEEE All-Society Periodicals Package (ASPP) 2005-present</collection><collection>IEEE All-Society Periodicals Package (ASPP) 1998-Present</collection><collection>IEEE Electronic Library (IEL)</collection><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Electronics &amp; 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In short-pulse experiments, the feasibility of the fabrication of coaxial cavity gyrotrons with an output power up to 2-MW, continuous wave (CW), has been demonstrated, and the information necessary for a technical design has been obtained. The development of a long-pulse 2-MW coaxial cavity gyrotron started within a European cooperation. In parallel to the design and fabrication of an industrial prototype gyrotron, a short-pulse preprototype gyrotron has been operated to verify the design of critical components. An output power of 1.2 MW with an efficiency of 20% has been achieved. The development of frequency tunable gyrotrons operating in the range from 105 to 140 GHz for stabilization of current driven plasma instabilities in fusion plasma devices (neoclassical tearing modes) is another task in the development of gyrotrons at the Forschungszentrum Karlsruhe.</abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/TPS.2006.872176</doi><tpages>14</tpages></addata></record>
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ispartof IEEE transactions on plasma science, 2006-04, Vol.34 (2), p.173-186
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1939-9375
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source IEEE Electronic Library (IEL)
subjects Applied sciences
Coaxial components
Coaxial gyrotron
Devices
diamond window
Electricity generation
Electron beams
Electron tubes
Electronic tubes, masers
Electronics
Electrons
Exact sciences and technology
Fabrication
frequency tuning
Fusion
gyrotron
Gyrotrons
high-power microwaves
Holes
Instability
Magnetic confinement and equilibrium
Particle beam measurements
Physics
Physics of gases, plasmas and electric discharges
Physics of plasmas and electric discharges
Plasma
Plasma devices
Plasma heating (beam injection, radio-frequency and microwave, ohmic, icr, ecr and current drive heating)
Plasma production and heating
Power generation
Pulse measurements
Pulsed power supplies
quasi-optical mode converter
Short pulses
single-stage depressed collector
Stabilization
Stellarators, torsatrons, heliacs, bumpy tori, and other toroidal confinement devices
step tunability
stray radiation
Tokamaks
Tubes
title High-power gyrotron development at Forschungszentrum Karlsruhe for fusion applications
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