Progress towards high-performance, steady-state spherical torus
Research on the spherical torus (or spherical tokamak) (ST) is being pursued to explore the scientific benefits of modifying the field line structure from that in more moderate aspect ratio devices, such as the conventional tokamak. The ST experiments are being conducted in various US research facil...
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Veröffentlicht in: | Plasma physics and controlled fusion 2003-12, Vol.45 (12A), p.A335-A350 |
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creator | Ono, M Bell, M G Bell, R E Bigelow, T Blanchard, W Boedo, J Bourdelle, C Bush, C Choe, W Chrzanowski, J Darrow, D S Diem, S J Doerner, R Efthimion, P C Garstka, G D Gates, D A Gray, T Grisham, L R Johnson, D W Kaita, R Kaye, S M Kessel, C Kissick, M W LeBlanc, B P Lee, K Lee, S G Lewicki, B T Luckhardt, S Maingi, R Majeski, R Manickam, J Maqueda, R Mau, T K Mazzucato, E Medley, S S Mueller, D Nishino, N Pacella, D Paoletti, F Park, H K Paul, S F Peng, Y-K M Phillips, C K Probert, P H Ramakrishnan, S Roquemore, A L Rosenberg, A Ryan, P M Sabbagh, S A Schooff, R J Skinner, C H Soukhanovskii, V Stutman, D Swain, D W Takase, Y Timberlake, J Tritz, K L Unterberg, E A Wilgen, J Williams, M Xu, X Zweben, S J Bialek, J M Blagojevic, B Carter, M D Davis, W Deng, B Dudek, L Ellis, R Finkenthal, M Foley, J Fredd, E Gibney, T Goldston, R J Hatcher, R E Hawryluk, R J Houlberg, W Harvey, R Ji, H Lowrance, J Lao, L L Levinton, F M Luhmann, N C Marsala, R Mastravito, D Menon, M M Mitarai, O Nagata, M Oliaro, G Parsells, R Peebles, T Piglowski, D Porter, G D Rensink, M Rewoldt, G Roney, P Shaing, K Stratton, B C Wampler, W R Wurden, G A |
description | Research on the spherical torus (or spherical tokamak) (ST) is being pursued to explore the scientific benefits of modifying the field line structure from that in more moderate aspect ratio devices, such as the conventional tokamak. The ST experiments are being conducted in various US research facilities including the MA-class National Spherical Torus Experiment (NSTX) at Princeton, and three medium sized ST research facilities: PEGASUS at University of Wisconsin, HIT-II at University of Washington, and CDX-U at Princeton. In the context of the fusion energy development path being formulated in the US, an ST-based Component Test Facility (CTF) and, ultimately a Demo device, are being discussed. For these, it is essential to develop high performance, steady-state operational scenarios. The relevant scientific issues are energy confinement, MHD stability at high beta (β), non-inductive sustainment, Ohmic-solenoid-free start-up, and power and particle handling. In the confinement area, the NSTX experiments have shown that the confinement can be up to 50% better than the ITER-98-pby2 H-mode scaling, consistent with the requirements for an ST-based CTF and Demo. In NSTX, CTF-relevant average toroidal beta values βT of up to 35% with a near unity central βT have been obtained. NSTX will be exploring advanced regimes where βT up to 40% can be sustained through active stabilization of resistive wall modes. To date, the most successful technique for non-inductive sustainment in NSTX is the high beta poloidal regime, where discharges with a high non-inductive fraction (~ 60% bootstrap current+NBI current drive) were sustained over the resistive skin time. Research on radio-frequency (RF) based heating and current drive utilizing high harmonic fast wave and electron Bernstein wave is also pursued on NSTX, PEGASUS, and CDX-U. For non-inductive start-up, the coaxial helicity injection, developed in HIT/HIT-II, has been adopted on NSTX to test the method up to Ip ~ 500 kA. In parallel, start-up using a RF current drive and only external poloidal field coils are being developed on NSTX. The area of power and particle handling is expected to be challenging because of the higher power density expected in the ST relative to that in conventional aspect-ratio tokamaks. Due to its promise for power and particle handling, liquid lithium is being studied in CDX-U as a potential plasma-facing surface for a fusion reactor. |
doi_str_mv | 10.1088/0741-3335/45/12A/022 |
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(PPPL), Princeton, NJ (United States)</creatorcontrib><description>Research on the spherical torus (or spherical tokamak) (ST) is being pursued to explore the scientific benefits of modifying the field line structure from that in more moderate aspect ratio devices, such as the conventional tokamak. The ST experiments are being conducted in various US research facilities including the MA-class National Spherical Torus Experiment (NSTX) at Princeton, and three medium sized ST research facilities: PEGASUS at University of Wisconsin, HIT-II at University of Washington, and CDX-U at Princeton. In the context of the fusion energy development path being formulated in the US, an ST-based Component Test Facility (CTF) and, ultimately a Demo device, are being discussed. For these, it is essential to develop high performance, steady-state operational scenarios. The relevant scientific issues are energy confinement, MHD stability at high beta (β), non-inductive sustainment, Ohmic-solenoid-free start-up, and power and particle handling. In the confinement area, the NSTX experiments have shown that the confinement can be up to 50% better than the ITER-98-pby2 H-mode scaling, consistent with the requirements for an ST-based CTF and Demo. In NSTX, CTF-relevant average toroidal beta values βT of up to 35% with a near unity central βT have been obtained. NSTX will be exploring advanced regimes where βT up to 40% can be sustained through active stabilization of resistive wall modes. To date, the most successful technique for non-inductive sustainment in NSTX is the high beta poloidal regime, where discharges with a high non-inductive fraction (~ 60% bootstrap current+NBI current drive) were sustained over the resistive skin time. Research on radio-frequency (RF) based heating and current drive utilizing high harmonic fast wave and electron Bernstein wave is also pursued on NSTX, PEGASUS, and CDX-U. For non-inductive start-up, the coaxial helicity injection, developed in HIT/HIT-II, has been adopted on NSTX to test the method up to Ip ~ 500 kA. In parallel, start-up using a RF current drive and only external poloidal field coils are being developed on NSTX. The area of power and particle handling is expected to be challenging because of the higher power density expected in the ST relative to that in conventional aspect-ratio tokamaks. Due to its promise for power and particle handling, liquid lithium is being studied in CDX-U as a potential plasma-facing surface for a fusion reactor.</description><identifier>ISSN: 0741-3335</identifier><identifier>EISSN: 1361-6587</identifier><identifier>DOI: 10.1088/0741-3335/45/12A/022</identifier><identifier>CODEN: PPCFET</identifier><language>eng</language><publisher>Bristol: IOP Publishing</publisher><ispartof>Plasma physics and controlled fusion, 2003-12, Vol.45 (12A), p.A335-A350</ispartof><rights>2004 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(PPPL), Princeton, NJ (United States)</creatorcontrib><title>Progress towards high-performance, steady-state spherical torus</title><title>Plasma physics and controlled fusion</title><description>Research on the spherical torus (or spherical tokamak) (ST) is being pursued to explore the scientific benefits of modifying the field line structure from that in more moderate aspect ratio devices, such as the conventional tokamak. The ST experiments are being conducted in various US research facilities including the MA-class National Spherical Torus Experiment (NSTX) at Princeton, and three medium sized ST research facilities: PEGASUS at University of Wisconsin, HIT-II at University of Washington, and CDX-U at Princeton. In the context of the fusion energy development path being formulated in the US, an ST-based Component Test Facility (CTF) and, ultimately a Demo device, are being discussed. For these, it is essential to develop high performance, steady-state operational scenarios. The relevant scientific issues are energy confinement, MHD stability at high beta (β), non-inductive sustainment, Ohmic-solenoid-free start-up, and power and particle handling. In the confinement area, the NSTX experiments have shown that the confinement can be up to 50% better than the ITER-98-pby2 H-mode scaling, consistent with the requirements for an ST-based CTF and Demo. In NSTX, CTF-relevant average toroidal beta values βT of up to 35% with a near unity central βT have been obtained. NSTX will be exploring advanced regimes where βT up to 40% can be sustained through active stabilization of resistive wall modes. To date, the most successful technique for non-inductive sustainment in NSTX is the high beta poloidal regime, where discharges with a high non-inductive fraction (~ 60% bootstrap current+NBI current drive) were sustained over the resistive skin time. Research on radio-frequency (RF) based heating and current drive utilizing high harmonic fast wave and electron Bernstein wave is also pursued on NSTX, PEGASUS, and CDX-U. For non-inductive start-up, the coaxial helicity injection, developed in HIT/HIT-II, has been adopted on NSTX to test the method up to Ip ~ 500 kA. In parallel, start-up using a RF current drive and only external poloidal field coils are being developed on NSTX. The area of power and particle handling is expected to be challenging because of the higher power density expected in the ST relative to that in conventional aspect-ratio tokamaks. 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Science</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>OTOTI</scope></search><sort><creationdate>20031201</creationdate><title>Progress towards high-performance, steady-state spherical torus</title><author>Ono, M ; Bell, M G ; Bell, R E ; Bigelow, T ; Blanchard, W ; Boedo, J ; Bourdelle, C ; Bush, C ; Choe, W ; Chrzanowski, J ; Darrow, D S ; Diem, S J ; Doerner, R ; Efthimion, P C ; Garstka, G D ; Gates, D A ; Gray, T ; Grisham, L R ; Johnson, D W ; Kaita, R ; Kaye, S M ; Kessel, C ; Kissick, M W ; LeBlanc, B P ; Lee, K ; Lee, S G ; Lewicki, B T ; Luckhardt, S ; Maingi, R ; Majeski, R ; Manickam, J ; Maqueda, R ; Mau, T K ; Mazzucato, E ; Medley, S S ; Mueller, D ; Nishino, N ; Pacella, D ; Paoletti, F ; Park, H K ; Paul, S F ; Peng, Y-K M ; Phillips, C K ; Probert, P H ; Ramakrishnan, S ; Roquemore, A L ; Rosenberg, A ; Ryan, P M ; Sabbagh, S A ; Schooff, R J ; Skinner, C H ; Soukhanovskii, V ; Stutman, D ; Swain, D W ; Takase, Y ; Timberlake, J ; Tritz, K L ; Unterberg, E A ; Wilgen, J ; Williams, M ; Xu, X ; Zweben, S J ; Bialek, J M ; Blagojevic, B ; Carter, M D ; Davis, W ; Deng, B ; Dudek, L ; Ellis, R ; Finkenthal, M ; Foley, J ; Fredd, E ; Gibney, T ; Goldston, R J ; Hatcher, R E ; Hawryluk, R J ; Houlberg, W ; Harvey, R ; Ji, H ; Lowrance, J ; Lao, L L ; Levinton, F M ; Luhmann, N C ; Marsala, R ; Mastravito, D ; Menon, M M ; Mitarai, O ; Nagata, M ; Oliaro, G ; Parsells, R ; Peebles, T ; Piglowski, D ; Porter, G D ; Rensink, M ; Rewoldt, G ; Roney, P ; Shaing, K ; Stratton, B C ; Wampler, W R ; Wurden, G A</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c494t-71680d0304217bf42dcd21692ada47878ebecb26685252d7eb50832624dafd2c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2003</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ono, M</creatorcontrib><creatorcontrib>Bell, M G</creatorcontrib><creatorcontrib>Bell, R E</creatorcontrib><creatorcontrib>Bigelow, T</creatorcontrib><creatorcontrib>Blanchard, W</creatorcontrib><creatorcontrib>Boedo, J</creatorcontrib><creatorcontrib>Bourdelle, C</creatorcontrib><creatorcontrib>Bush, C</creatorcontrib><creatorcontrib>Choe, W</creatorcontrib><creatorcontrib>Chrzanowski, J</creatorcontrib><creatorcontrib>Darrow, D S</creatorcontrib><creatorcontrib>Diem, S J</creatorcontrib><creatorcontrib>Doerner, R</creatorcontrib><creatorcontrib>Efthimion, P C</creatorcontrib><creatorcontrib>Garstka, G D</creatorcontrib><creatorcontrib>Gates, D A</creatorcontrib><creatorcontrib>Gray, T</creatorcontrib><creatorcontrib>Grisham, L R</creatorcontrib><creatorcontrib>Johnson, D W</creatorcontrib><creatorcontrib>Kaita, R</creatorcontrib><creatorcontrib>Kaye, S M</creatorcontrib><creatorcontrib>Kessel, C</creatorcontrib><creatorcontrib>Kissick, M W</creatorcontrib><creatorcontrib>LeBlanc, B P</creatorcontrib><creatorcontrib>Lee, K</creatorcontrib><creatorcontrib>Lee, S G</creatorcontrib><creatorcontrib>Lewicki, B T</creatorcontrib><creatorcontrib>Luckhardt, S</creatorcontrib><creatorcontrib>Maingi, R</creatorcontrib><creatorcontrib>Majeski, R</creatorcontrib><creatorcontrib>Manickam, J</creatorcontrib><creatorcontrib>Maqueda, R</creatorcontrib><creatorcontrib>Mau, T K</creatorcontrib><creatorcontrib>Mazzucato, E</creatorcontrib><creatorcontrib>Medley, S S</creatorcontrib><creatorcontrib>Mueller, D</creatorcontrib><creatorcontrib>Nishino, N</creatorcontrib><creatorcontrib>Pacella, D</creatorcontrib><creatorcontrib>Paoletti, F</creatorcontrib><creatorcontrib>Park, H K</creatorcontrib><creatorcontrib>Paul, S F</creatorcontrib><creatorcontrib>Peng, Y-K M</creatorcontrib><creatorcontrib>Phillips, C K</creatorcontrib><creatorcontrib>Probert, P H</creatorcontrib><creatorcontrib>Ramakrishnan, S</creatorcontrib><creatorcontrib>Roquemore, A L</creatorcontrib><creatorcontrib>Rosenberg, 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M</creatorcontrib><creatorcontrib>Foley, J</creatorcontrib><creatorcontrib>Fredd, E</creatorcontrib><creatorcontrib>Gibney, T</creatorcontrib><creatorcontrib>Goldston, R J</creatorcontrib><creatorcontrib>Hatcher, R E</creatorcontrib><creatorcontrib>Hawryluk, R J</creatorcontrib><creatorcontrib>Houlberg, W</creatorcontrib><creatorcontrib>Harvey, R</creatorcontrib><creatorcontrib>Ji, H</creatorcontrib><creatorcontrib>Lowrance, J</creatorcontrib><creatorcontrib>Lao, L L</creatorcontrib><creatorcontrib>Levinton, F M</creatorcontrib><creatorcontrib>Luhmann, N C</creatorcontrib><creatorcontrib>Marsala, R</creatorcontrib><creatorcontrib>Mastravito, D</creatorcontrib><creatorcontrib>Menon, M M</creatorcontrib><creatorcontrib>Mitarai, O</creatorcontrib><creatorcontrib>Nagata, M</creatorcontrib><creatorcontrib>Oliaro, G</creatorcontrib><creatorcontrib>Parsells, R</creatorcontrib><creatorcontrib>Peebles, T</creatorcontrib><creatorcontrib>Piglowski, D</creatorcontrib><creatorcontrib>Porter, G D</creatorcontrib><creatorcontrib>Rensink, M</creatorcontrib><creatorcontrib>Rewoldt, G</creatorcontrib><creatorcontrib>Roney, P</creatorcontrib><creatorcontrib>Shaing, K</creatorcontrib><creatorcontrib>Stratton, B C</creatorcontrib><creatorcontrib>Wampler, W R</creatorcontrib><creatorcontrib>Wurden, G A</creatorcontrib><creatorcontrib>Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States)</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>Plasma physics and controlled fusion</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ono, M</au><au>Bell, M G</au><au>Bell, R E</au><au>Bigelow, T</au><au>Blanchard, W</au><au>Boedo, J</au><au>Bourdelle, C</au><au>Bush, C</au><au>Choe, W</au><au>Chrzanowski, J</au><au>Darrow, D S</au><au>Diem, S J</au><au>Doerner, R</au><au>Efthimion, P C</au><au>Garstka, G D</au><au>Gates, D A</au><au>Gray, T</au><au>Grisham, L R</au><au>Johnson, D W</au><au>Kaita, R</au><au>Kaye, S M</au><au>Kessel, C</au><au>Kissick, M W</au><au>LeBlanc, B P</au><au>Lee, K</au><au>Lee, S G</au><au>Lewicki, B T</au><au>Luckhardt, S</au><au>Maingi, R</au><au>Majeski, R</au><au>Manickam, J</au><au>Maqueda, R</au><au>Mau, T K</au><au>Mazzucato, E</au><au>Medley, S S</au><au>Mueller, D</au><au>Nishino, N</au><au>Pacella, D</au><au>Paoletti, F</au><au>Park, H K</au><au>Paul, S F</au><au>Peng, Y-K M</au><au>Phillips, C K</au><au>Probert, P H</au><au>Ramakrishnan, S</au><au>Roquemore, A L</au><au>Rosenberg, A</au><au>Ryan, P M</au><au>Sabbagh, S A</au><au>Schooff, R J</au><au>Skinner, C H</au><au>Soukhanovskii, V</au><au>Stutman, D</au><au>Swain, D W</au><au>Takase, Y</au><au>Timberlake, J</au><au>Tritz, K L</au><au>Unterberg, E A</au><au>Wilgen, J</au><au>Williams, M</au><au>Xu, X</au><au>Zweben, S J</au><au>Bialek, J M</au><au>Blagojevic, B</au><au>Carter, M D</au><au>Davis, W</au><au>Deng, B</au><au>Dudek, L</au><au>Ellis, R</au><au>Finkenthal, M</au><au>Foley, J</au><au>Fredd, E</au><au>Gibney, T</au><au>Goldston, R J</au><au>Hatcher, R E</au><au>Hawryluk, R J</au><au>Houlberg, W</au><au>Harvey, R</au><au>Ji, H</au><au>Lowrance, J</au><au>Lao, L L</au><au>Levinton, F M</au><au>Luhmann, N C</au><au>Marsala, R</au><au>Mastravito, D</au><au>Menon, M M</au><au>Mitarai, O</au><au>Nagata, M</au><au>Oliaro, G</au><au>Parsells, R</au><au>Peebles, T</au><au>Piglowski, D</au><au>Porter, G D</au><au>Rensink, M</au><au>Rewoldt, G</au><au>Roney, P</au><au>Shaing, K</au><au>Stratton, B C</au><au>Wampler, W R</au><au>Wurden, G A</au><aucorp>Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Progress towards high-performance, steady-state spherical torus</atitle><jtitle>Plasma physics and controlled fusion</jtitle><date>2003-12-01</date><risdate>2003</risdate><volume>45</volume><issue>12A</issue><spage>A335</spage><epage>A350</epage><pages>A335-A350</pages><issn>0741-3335</issn><eissn>1361-6587</eissn><coden>PPCFET</coden><abstract>Research on the spherical torus (or spherical tokamak) (ST) is being pursued to explore the scientific benefits of modifying the field line structure from that in more moderate aspect ratio devices, such as the conventional tokamak. The ST experiments are being conducted in various US research facilities including the MA-class National Spherical Torus Experiment (NSTX) at Princeton, and three medium sized ST research facilities: PEGASUS at University of Wisconsin, HIT-II at University of Washington, and CDX-U at Princeton. In the context of the fusion energy development path being formulated in the US, an ST-based Component Test Facility (CTF) and, ultimately a Demo device, are being discussed. For these, it is essential to develop high performance, steady-state operational scenarios. The relevant scientific issues are energy confinement, MHD stability at high beta (β), non-inductive sustainment, Ohmic-solenoid-free start-up, and power and particle handling. In the confinement area, the NSTX experiments have shown that the confinement can be up to 50% better than the ITER-98-pby2 H-mode scaling, consistent with the requirements for an ST-based CTF and Demo. In NSTX, CTF-relevant average toroidal beta values βT of up to 35% with a near unity central βT have been obtained. NSTX will be exploring advanced regimes where βT up to 40% can be sustained through active stabilization of resistive wall modes. To date, the most successful technique for non-inductive sustainment in NSTX is the high beta poloidal regime, where discharges with a high non-inductive fraction (~ 60% bootstrap current+NBI current drive) were sustained over the resistive skin time. Research on radio-frequency (RF) based heating and current drive utilizing high harmonic fast wave and electron Bernstein wave is also pursued on NSTX, PEGASUS, and CDX-U. For non-inductive start-up, the coaxial helicity injection, developed in HIT/HIT-II, has been adopted on NSTX to test the method up to Ip ~ 500 kA. In parallel, start-up using a RF current drive and only external poloidal field coils are being developed on NSTX. The area of power and particle handling is expected to be challenging because of the higher power density expected in the ST relative to that in conventional aspect-ratio tokamaks. Due to its promise for power and particle handling, liquid lithium is being studied in CDX-U as a potential plasma-facing surface for a fusion reactor.</abstract><cop>Bristol</cop><pub>IOP Publishing</pub><doi>10.1088/0741-3335/45/12A/022</doi><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0741-3335 |
ispartof | Plasma physics and controlled fusion, 2003-12, Vol.45 (12A), p.A335-A350 |
issn | 0741-3335 1361-6587 |
language | eng |
recordid | cdi_osti_scitechconnect_1081822 |
source | IOP Publishing Journals; Institute of Physics (IOP) Journals - HEAL-Link |
title | Progress towards high-performance, steady-state spherical torus |
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