Exploring drift effects in TCV single-null plasmas with the UEDGE code
This paper explores the effects of particle drifts across the magnetic field in TCV single-null plasmas using the two-dimensional edge plasma transport code UEDGE. In particular, it aims to reproduce a double-peaked density target profile, a feature which has been observed both at JET and in a TCV f...
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Veröffentlicht in: | Plasma physics and controlled fusion 2017-10, Vol.59 (10), p.105004 |
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description | This paper explores the effects of particle drifts across the magnetic field in TCV single-null plasmas using the two-dimensional edge plasma transport code UEDGE. In particular, it aims to reproduce a double-peaked density target profile, a feature which has been observed both at JET and in a TCV forward-field ( ∇ B drift of core ions towards the X-point) discharge. Initial simulations are performed with drift effects turned off. This allows identification of the input parameters that strongly influence the computed steady-state but are not well known from the experiment. Including cross-field drifts self-consistently in the simulations brings computed profiles at the inner target closer to the experiment, with the double peak being reproduced for the density. In agreement with the experiment, simulations of a similar reversed-field shot yield lower ne and higher Te at the inner target, as well as unchanged temperatures at the outer plate. However, several discrepancies remain. In the forward field case, the inner target density peak near the separatrix is much sharper than seen experimentally. Furthermore, simulations show a strong dependence of the outer plate density and of the outer/inner power sharing on toroidal field direction. Experimentally, no such dependencies are observed. In the simulations, the changes of target profiles with field direction are mainly due to E × B drifts in the divertor region. While these simulations highlight the importance of E × B drifts in these TCV plasmas, the remaining differences with the experiment indicate that their role is overestimated in the simulations. |
doi_str_mv | 10.1088/1361-6587/aa7c8e |
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(LLNL), Livermore, CA (United States) ; École Polytechnique Fédérale de Lausanne (EPFL) (Switzlerland)</creatorcontrib><description>This paper explores the effects of particle drifts across the magnetic field in TCV single-null plasmas using the two-dimensional edge plasma transport code UEDGE. In particular, it aims to reproduce a double-peaked density target profile, a feature which has been observed both at JET and in a TCV forward-field ( ∇ B drift of core ions towards the X-point) discharge. Initial simulations are performed with drift effects turned off. This allows identification of the input parameters that strongly influence the computed steady-state but are not well known from the experiment. Including cross-field drifts self-consistently in the simulations brings computed profiles at the inner target closer to the experiment, with the double peak being reproduced for the density. In agreement with the experiment, simulations of a similar reversed-field shot yield lower ne and higher Te at the inner target, as well as unchanged temperatures at the outer plate. However, several discrepancies remain. In the forward field case, the inner target density peak near the separatrix is much sharper than seen experimentally. Furthermore, simulations show a strong dependence of the outer plate density and of the outer/inner power sharing on toroidal field direction. Experimentally, no such dependencies are observed. In the simulations, the changes of target profiles with field direction are mainly due to E × B drifts in the divertor region. While these simulations highlight the importance of E × B drifts in these TCV plasmas, the remaining differences with the experiment indicate that their role is overestimated in the simulations.</description><identifier>ISSN: 0741-3335</identifier><identifier>EISSN: 1361-6587</identifier><identifier>DOI: 10.1088/1361-6587/aa7c8e</identifier><identifier>CODEN: PLPHBZ</identifier><language>eng</language><publisher>United States: IOP Publishing</publisher><subject>70 PLASMA PHYSICS AND FUSION TECHNOLOGY ; drifts ; single-null ; TCV ; UEDGE</subject><ispartof>Plasma physics and controlled fusion, 2017-10, Vol.59 (10), p.105004</ispartof><rights>2017 IOP Publishing Ltd</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c430t-bb8d336ad82419ff9b11f0d80e7cb8ed0780d4d4b6b4579fcfce312c1faf4c0e3</citedby><cites>FETCH-LOGICAL-c430t-bb8d336ad82419ff9b11f0d80e7cb8ed0780d4d4b6b4579fcfce312c1faf4c0e3</cites><orcidid>0000-0003-3926-1374 ; 0000000339261374</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://iopscience.iop.org/article/10.1088/1361-6587/aa7c8e/pdf$$EPDF$$P50$$Giop$$H</linktopdf><link.rule.ids>230,314,780,784,885,27924,27925,53846,53893</link.rule.ids><backlink>$$Uhttps://www.osti.gov/servlets/purl/1465288$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Christen, N</creatorcontrib><creatorcontrib>Theiler, C</creatorcontrib><creatorcontrib>Rognlien, TD</creatorcontrib><creatorcontrib>Rensink, ME</creatorcontrib><creatorcontrib>Reimerdes, H</creatorcontrib><creatorcontrib>Maurizio, R</creatorcontrib><creatorcontrib>Labit, B</creatorcontrib><creatorcontrib>Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)</creatorcontrib><creatorcontrib>École Polytechnique Fédérale de Lausanne (EPFL) (Switzlerland)</creatorcontrib><title>Exploring drift effects in TCV single-null plasmas with the UEDGE code</title><title>Plasma physics and controlled fusion</title><addtitle>PPCF</addtitle><addtitle>Plasma Phys. Control. Fusion</addtitle><description>This paper explores the effects of particle drifts across the magnetic field in TCV single-null plasmas using the two-dimensional edge plasma transport code UEDGE. In particular, it aims to reproduce a double-peaked density target profile, a feature which has been observed both at JET and in a TCV forward-field ( ∇ B drift of core ions towards the X-point) discharge. Initial simulations are performed with drift effects turned off. This allows identification of the input parameters that strongly influence the computed steady-state but are not well known from the experiment. Including cross-field drifts self-consistently in the simulations brings computed profiles at the inner target closer to the experiment, with the double peak being reproduced for the density. In agreement with the experiment, simulations of a similar reversed-field shot yield lower ne and higher Te at the inner target, as well as unchanged temperatures at the outer plate. However, several discrepancies remain. In the forward field case, the inner target density peak near the separatrix is much sharper than seen experimentally. Furthermore, simulations show a strong dependence of the outer plate density and of the outer/inner power sharing on toroidal field direction. Experimentally, no such dependencies are observed. In the simulations, the changes of target profiles with field direction are mainly due to E × B drifts in the divertor region. While these simulations highlight the importance of E × B drifts in these TCV plasmas, the remaining differences with the experiment indicate that their role is overestimated in the simulations.</description><subject>70 PLASMA PHYSICS AND FUSION TECHNOLOGY</subject><subject>drifts</subject><subject>single-null</subject><subject>TCV</subject><subject>UEDGE</subject><issn>0741-3335</issn><issn>1361-6587</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNp9kM9LwzAUx4MoOKd3j8GbYN1Lk7bpUWY3hYGXzWtI88NldG1JMnT_vR0VT-LpwXuf7-O9D0K3BB4JcD4jNCdJnvFiJmWhuDlDk9_WOZpAwUhCKc0u0VUIOwBCeJpP0KL66pvOu_YDa-9sxMZao2LArsXr-TsOw6QxSXtoGtw3MuxlwJ8ubnHcGrypnpcVVp021-jCyiaYm586RZtFtZ6_JKu35ev8aZUoRiEmdc01pbnUPGWktLasCbGgOZhC1dxoKDhoplmd1ywrSqusMpSkilhpmQJDp-hu3NuF6ERQLhq1VV3bDjcLwvIs5XyAYISU70Lwxoreu730R0FAnGSJkxlxMiNGWUPkYYy4rhe77uDb4Yv_8Ps_8L5XVmTlGMsAmOi1pd8d6nj4</recordid><startdate>20171001</startdate><enddate>20171001</enddate><creator>Christen, N</creator><creator>Theiler, C</creator><creator>Rognlien, TD</creator><creator>Rensink, ME</creator><creator>Reimerdes, H</creator><creator>Maurizio, R</creator><creator>Labit, B</creator><general>IOP Publishing</general><general>IOP Science</general><scope>AAYXX</scope><scope>CITATION</scope><scope>OIOZB</scope><scope>OTOTI</scope><orcidid>https://orcid.org/0000-0003-3926-1374</orcidid><orcidid>https://orcid.org/0000000339261374</orcidid></search><sort><creationdate>20171001</creationdate><title>Exploring drift effects in TCV single-null plasmas with the UEDGE code</title><author>Christen, N ; Theiler, C ; Rognlien, TD ; Rensink, ME ; Reimerdes, H ; Maurizio, R ; Labit, B</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c430t-bb8d336ad82419ff9b11f0d80e7cb8ed0780d4d4b6b4579fcfce312c1faf4c0e3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>70 PLASMA PHYSICS AND FUSION TECHNOLOGY</topic><topic>drifts</topic><topic>single-null</topic><topic>TCV</topic><topic>UEDGE</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Christen, N</creatorcontrib><creatorcontrib>Theiler, C</creatorcontrib><creatorcontrib>Rognlien, TD</creatorcontrib><creatorcontrib>Rensink, ME</creatorcontrib><creatorcontrib>Reimerdes, H</creatorcontrib><creatorcontrib>Maurizio, R</creatorcontrib><creatorcontrib>Labit, B</creatorcontrib><creatorcontrib>Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)</creatorcontrib><creatorcontrib>École Polytechnique Fédérale de Lausanne (EPFL) (Switzlerland)</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV - Hybrid</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>Christen, N</au><au>Theiler, C</au><au>Rognlien, TD</au><au>Rensink, ME</au><au>Reimerdes, H</au><au>Maurizio, R</au><au>Labit, B</au><aucorp>Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)</aucorp><aucorp>École Polytechnique Fédérale de Lausanne (EPFL) (Switzlerland)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Exploring drift effects in TCV single-null plasmas with the UEDGE code</atitle><jtitle>Plasma physics and controlled fusion</jtitle><stitle>PPCF</stitle><addtitle>Plasma Phys. Control. Fusion</addtitle><date>2017-10-01</date><risdate>2017</risdate><volume>59</volume><issue>10</issue><spage>105004</spage><pages>105004-</pages><issn>0741-3335</issn><eissn>1361-6587</eissn><coden>PLPHBZ</coden><abstract>This paper explores the effects of particle drifts across the magnetic field in TCV single-null plasmas using the two-dimensional edge plasma transport code UEDGE. In particular, it aims to reproduce a double-peaked density target profile, a feature which has been observed both at JET and in a TCV forward-field ( ∇ B drift of core ions towards the X-point) discharge. Initial simulations are performed with drift effects turned off. This allows identification of the input parameters that strongly influence the computed steady-state but are not well known from the experiment. Including cross-field drifts self-consistently in the simulations brings computed profiles at the inner target closer to the experiment, with the double peak being reproduced for the density. In agreement with the experiment, simulations of a similar reversed-field shot yield lower ne and higher Te at the inner target, as well as unchanged temperatures at the outer plate. However, several discrepancies remain. In the forward field case, the inner target density peak near the separatrix is much sharper than seen experimentally. Furthermore, simulations show a strong dependence of the outer plate density and of the outer/inner power sharing on toroidal field direction. Experimentally, no such dependencies are observed. In the simulations, the changes of target profiles with field direction are mainly due to E × B drifts in the divertor region. While these simulations highlight the importance of E × B drifts in these TCV plasmas, the remaining differences with the experiment indicate that their role is overestimated in the simulations.</abstract><cop>United States</cop><pub>IOP Publishing</pub><doi>10.1088/1361-6587/aa7c8e</doi><tpages>15</tpages><orcidid>https://orcid.org/0000-0003-3926-1374</orcidid><orcidid>https://orcid.org/0000000339261374</orcidid><oa>free_for_read</oa></addata></record> |
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title | Exploring drift effects in TCV single-null plasmas with the UEDGE code |
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