F Bagnato, B P Duval, O Sauter, S Coda, A Karpushov, A Merle, B Labit, O Fevrier, A Pau, D Mykytchuk, L Porte, J Ball
{"title":"TCV 托卡马克负三角中的杂质 C 输运和等离子体旋转研究","authors":"F Bagnato, B P Duval, O Sauter, S Coda, A Karpushov, A Merle, B Labit, O Fevrier, A Pau, D Mykytchuk, L Porte, J Ball","doi":"10.1088/1361-6587/ad5229","DOIUrl":null,"url":null,"abstract":"Carbon impurity transport is studied in the TCV tokamak using a charge exchange recombination diagnostic. TCVs flexible shaping capabilities were exploited to extend previous impurity transport studies to negative triangularity (<italic toggle=\"yes\">δ</italic> < 0). A practical way of studying light impurity transport (like C, TCVs main impurity species due to graphite tiled walls) is to investigate the correlations between the impurity ion gradients that, in this study, highlighted significant differences between positive (PT) and negative <italic toggle=\"yes\">δ</italic> (NT) plasma configurations. <italic toggle=\"yes\">δ</italic> scans (<inline-formula>\n<tex-math><?CDATA $-0.6\\lt\\delta\\lt +0.6$?></tex-math>\n<mml:math overflow=\"scroll\"><mml:mrow><mml:mo>−</mml:mo><mml:mn>0.6</mml:mn><mml:mo><</mml:mo><mml:mi>δ</mml:mi><mml:mo><</mml:mo><mml:mo>+</mml:mo><mml:mn>0.6</mml:mn></mml:mrow></mml:math>\n<inline-graphic xlink:href=\"ppcfad5229ieqn1.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula>) were performed in limited configurations, but displayed little correlation between C temperature, rotation and density gradients for positive <italic toggle=\"yes\">δ</italic>. This stiff response for <italic toggle=\"yes\">δ</italic> > 0 changes for negative <italic toggle=\"yes\">δ</italic>, where the evolution of <inline-formula>\n<tex-math><?CDATA $\\nabla v_\\mathrm{tor}$?></tex-math>\n<mml:math overflow=\"scroll\"><mml:mrow><mml:mi mathvariant=\"normal\">∇</mml:mi><mml:msub><mml:mi>v</mml:mi><mml:mrow><mml:mi>tor</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>\n<inline-graphic xlink:href=\"ppcfad5229ieqn2.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> was accompanied by variations of <inline-formula>\n<tex-math><?CDATA $\\nabla n_\\mathrm{C}$?></tex-math>\n<mml:math overflow=\"scroll\"><mml:mrow><mml:mi mathvariant=\"normal\">∇</mml:mi><mml:msub><mml:mi>n</mml:mi><mml:mrow><mml:mi mathvariant=\"normal\">C</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>\n<inline-graphic xlink:href=\"ppcfad5229ieqn3.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> over a range of negative <italic toggle=\"yes\">δ</italic>, showing that transport, in NT, is affected by velocity gradients. Similar <italic toggle=\"yes\">δ</italic> scans were performed with additional NBH (Neutral Beam Heating), with power steps ranging from 0.25 MW to 1.25 MW, highlighting increased momentum confinement in negative <italic toggle=\"yes\">δ</italic>. Finally, the evolution of intrinsic plasma toroidal rotation across linear to saturated ohmic confinement regime (LOC/SOC) transitions was explored at <italic toggle=\"yes\">δ</italic> < 0, expanding previous studies performed in TCV for <inline-formula>\n<tex-math><?CDATA $\\delta \\gt $?></tex-math>\n<mml:math overflow=\"scroll\"><mml:mrow><mml:mi>δ</mml:mi><mml:mo>></mml:mo></mml:mrow></mml:math>\n<inline-graphic xlink:href=\"ppcfad5229ieqn4.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> 0 (Bagnato <italic toggle=\"yes\">et al</italic> 2023 <italic toggle=\"yes\">Nucl. Fusion</italic>\n<bold>63</bold> 056006). Toroidal rotation reversal was not observed for <italic toggle=\"yes\">δ</italic> < 0, despite clear LOC/SOC transitions, confirming that these two phenomena occur concomitantly only in a restricted number of cases and under specific conditions.","PeriodicalId":20239,"journal":{"name":"Plasma Physics and Controlled Fusion","volume":"21 1","pages":""},"PeriodicalIF":2.1000,"publicationDate":"2024-06-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Study of impurity C transport and plasma rotation in negative triangularity on the TCV tokamak\",\"authors\":\"F Bagnato, B P Duval, O Sauter, S Coda, A Karpushov, A Merle, B Labit, O Fevrier, A Pau, D Mykytchuk, L Porte, J Ball\",\"doi\":\"10.1088/1361-6587/ad5229\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Carbon impurity transport is studied in the TCV tokamak using a charge exchange recombination diagnostic. TCVs flexible shaping capabilities were exploited to extend previous impurity transport studies to negative triangularity (<italic toggle=\\\"yes\\\">δ</italic> < 0). A practical way of studying light impurity transport (like C, TCVs main impurity species due to graphite tiled walls) is to investigate the correlations between the impurity ion gradients that, in this study, highlighted significant differences between positive (PT) and negative <italic toggle=\\\"yes\\\">δ</italic> (NT) plasma configurations. <italic toggle=\\\"yes\\\">δ</italic> scans (<inline-formula>\\n<tex-math><?CDATA $-0.6\\\\lt\\\\delta\\\\lt +0.6$?></tex-math>\\n<mml:math overflow=\\\"scroll\\\"><mml:mrow><mml:mo>−</mml:mo><mml:mn>0.6</mml:mn><mml:mo><</mml:mo><mml:mi>δ</mml:mi><mml:mo><</mml:mo><mml:mo>+</mml:mo><mml:mn>0.6</mml:mn></mml:mrow></mml:math>\\n<inline-graphic xlink:href=\\\"ppcfad5229ieqn1.gif\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula>) were performed in limited configurations, but displayed little correlation between C temperature, rotation and density gradients for positive <italic toggle=\\\"yes\\\">δ</italic>. This stiff response for <italic toggle=\\\"yes\\\">δ</italic> > 0 changes for negative <italic toggle=\\\"yes\\\">δ</italic>, where the evolution of <inline-formula>\\n<tex-math><?CDATA $\\\\nabla v_\\\\mathrm{tor}$?></tex-math>\\n<mml:math overflow=\\\"scroll\\\"><mml:mrow><mml:mi mathvariant=\\\"normal\\\">∇</mml:mi><mml:msub><mml:mi>v</mml:mi><mml:mrow><mml:mi>tor</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>\\n<inline-graphic xlink:href=\\\"ppcfad5229ieqn2.gif\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> was accompanied by variations of <inline-formula>\\n<tex-math><?CDATA $\\\\nabla n_\\\\mathrm{C}$?></tex-math>\\n<mml:math overflow=\\\"scroll\\\"><mml:mrow><mml:mi mathvariant=\\\"normal\\\">∇</mml:mi><mml:msub><mml:mi>n</mml:mi><mml:mrow><mml:mi mathvariant=\\\"normal\\\">C</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>\\n<inline-graphic xlink:href=\\\"ppcfad5229ieqn3.gif\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> over a range of negative <italic toggle=\\\"yes\\\">δ</italic>, showing that transport, in NT, is affected by velocity gradients. Similar <italic toggle=\\\"yes\\\">δ</italic> scans were performed with additional NBH (Neutral Beam Heating), with power steps ranging from 0.25 MW to 1.25 MW, highlighting increased momentum confinement in negative <italic toggle=\\\"yes\\\">δ</italic>. Finally, the evolution of intrinsic plasma toroidal rotation across linear to saturated ohmic confinement regime (LOC/SOC) transitions was explored at <italic toggle=\\\"yes\\\">δ</italic> < 0, expanding previous studies performed in TCV for <inline-formula>\\n<tex-math><?CDATA $\\\\delta \\\\gt $?></tex-math>\\n<mml:math overflow=\\\"scroll\\\"><mml:mrow><mml:mi>δ</mml:mi><mml:mo>></mml:mo></mml:mrow></mml:math>\\n<inline-graphic xlink:href=\\\"ppcfad5229ieqn4.gif\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> 0 (Bagnato <italic toggle=\\\"yes\\\">et al</italic> 2023 <italic toggle=\\\"yes\\\">Nucl. Fusion</italic>\\n<bold>63</bold> 056006). Toroidal rotation reversal was not observed for <italic toggle=\\\"yes\\\">δ</italic> < 0, despite clear LOC/SOC transitions, confirming that these two phenomena occur concomitantly only in a restricted number of cases and under specific conditions.\",\"PeriodicalId\":20239,\"journal\":{\"name\":\"Plasma Physics and Controlled Fusion\",\"volume\":\"21 1\",\"pages\":\"\"},\"PeriodicalIF\":2.1000,\"publicationDate\":\"2024-06-07\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Plasma Physics and Controlled Fusion\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1088/1361-6587/ad5229\",\"RegionNum\":2,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, FLUIDS & PLASMAS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Plasma Physics and Controlled Fusion","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1088/1361-6587/ad5229","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, FLUIDS & PLASMAS","Score":null,"Total":0}
Study of impurity C transport and plasma rotation in negative triangularity on the TCV tokamak
Carbon impurity transport is studied in the TCV tokamak using a charge exchange recombination diagnostic. TCVs flexible shaping capabilities were exploited to extend previous impurity transport studies to negative triangularity (δ < 0). A practical way of studying light impurity transport (like C, TCVs main impurity species due to graphite tiled walls) is to investigate the correlations between the impurity ion gradients that, in this study, highlighted significant differences between positive (PT) and negative δ (NT) plasma configurations. δ scans (−0.6<δ<+0.6) were performed in limited configurations, but displayed little correlation between C temperature, rotation and density gradients for positive δ. This stiff response for δ > 0 changes for negative δ, where the evolution of ∇vtor was accompanied by variations of ∇nC over a range of negative δ, showing that transport, in NT, is affected by velocity gradients. Similar δ scans were performed with additional NBH (Neutral Beam Heating), with power steps ranging from 0.25 MW to 1.25 MW, highlighting increased momentum confinement in negative δ. Finally, the evolution of intrinsic plasma toroidal rotation across linear to saturated ohmic confinement regime (LOC/SOC) transitions was explored at δ < 0, expanding previous studies performed in TCV for δ> 0 (Bagnato et al 2023 Nucl. Fusion63 056006). Toroidal rotation reversal was not observed for δ < 0, despite clear LOC/SOC transitions, confirming that these two phenomena occur concomitantly only in a restricted number of cases and under specific conditions.
期刊介绍:
Plasma Physics and Controlled Fusion covers all aspects of the physics of hot, highly ionised plasmas. This includes results of current experimental and theoretical research on all aspects of the physics of high-temperature plasmas and of controlled nuclear fusion, including the basic phenomena in highly-ionised gases in the laboratory, in the ionosphere and in space, in magnetic-confinement and inertial-confinement fusion as well as related diagnostic methods.
Papers with a technological emphasis, for example in such topics as plasma control, fusion technology and diagnostics, are welcomed when the plasma physics is an integral part of the paper or when the technology is unique to plasma applications or new to the field of plasma physics. Papers on dusty plasma physics are welcome when there is a clear relevance to fusion.