Evaluation of edge transport and core accumulation of tungsten for CFETR with EMC3-EIRENE and STRAHL
The edge transport and core accumulation of tungsten (W) particles on China Fusion Engineering Test Reactor (CFETR) have been studied by integrated modelling consisting of EMC3-EIRENE and STRAHL codes. The edge transport and power dissipation of W particles are simulated by EMC3-EIRENE. An in–out as...
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description | The edge transport and core accumulation of tungsten (W) particles on China Fusion Engineering Test Reactor (CFETR) have been studied by integrated modelling consisting of EMC3-EIRENE and STRAHL codes. The edge transport and power dissipation of W particles are simulated by EMC3-EIRENE. An in–out asymmetry of W
(1–28)+
ions density has been revealed in the in- and out-board divertor regions. This is mainly due to the stronger reversal flow velocity of W ions at the outboard divertor. The upward flow of W ions near the separatrix leads to a moderate W impurity leakage from the divertor on CFETR compared to the existing full W device ASDEX Upgrade due to the high plasma density near the CFETR divertor targets. Further, the density distribution and radiation loss of W ions in the core region are investigated by STRAHL code. The high charge-state W
(29–60)+
and W
(61–74)+
ions mainly reside in the regions of Ψ
N
= 0.20–0.98 and 0.00–0.90 (Ψ
N
is the normalized poloidal magnetic flux), respectively. The W induced energy dissipation in different regions is assessed according to both STRAHL and EMC3-EIRENE simulations. Particularly, the impacts of the W core radiation on the operation regime are discussed according to the H-mode threshold scaling law proposed by Martin
et al
(2008
J. Phys.: Conf. Ser.
123
012033) for the baseline plasma on CFETR. Further, parameter studies on the pinch velocity (
v
imp
) and diffusion coefficient (
D
imp
) have been performed to check their impacts on the operation regime of CFETR. A three-fold increase of
v
imp
/
D
imp
results in a higher W core energy loss, which can lead to the transition from H-mode back to L-mode. |
doi_str_mv | 10.1088/1741-4326/ac95aa |
format | Article |
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(1–28)+
ions density has been revealed in the in- and out-board divertor regions. This is mainly due to the stronger reversal flow velocity of W ions at the outboard divertor. The upward flow of W ions near the separatrix leads to a moderate W impurity leakage from the divertor on CFETR compared to the existing full W device ASDEX Upgrade due to the high plasma density near the CFETR divertor targets. Further, the density distribution and radiation loss of W ions in the core region are investigated by STRAHL code. The high charge-state W
(29–60)+
and W
(61–74)+
ions mainly reside in the regions of Ψ
N
= 0.20–0.98 and 0.00–0.90 (Ψ
N
is the normalized poloidal magnetic flux), respectively. The W induced energy dissipation in different regions is assessed according to both STRAHL and EMC3-EIRENE simulations. Particularly, the impacts of the W core radiation on the operation regime are discussed according to the H-mode threshold scaling law proposed by Martin
et al
(2008
J. Phys.: Conf. Ser.
123
012033) for the baseline plasma on CFETR. Further, parameter studies on the pinch velocity (
v
imp
) and diffusion coefficient (
D
imp
) have been performed to check their impacts on the operation regime of CFETR. A three-fold increase of
v
imp
/
D
imp
results in a higher W core energy loss, which can lead to the transition from H-mode back to L-mode.</description><identifier>ISSN: 0029-5515</identifier><identifier>EISSN: 1741-4326</identifier><identifier>DOI: 10.1088/1741-4326/ac95aa</identifier><identifier>CODEN: NUFUAU</identifier><language>eng</language><publisher>IOP Publishing</publisher><subject>CFETR ; EMC3-EIRENE ; STRAHL ; tungsten distribution</subject><ispartof>Nuclear fusion, 2022-12, Vol.62 (12), p.126040</ispartof><rights>2022 IAEA, Vienna</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c312t-cb0b538038fec6ea7f90ca749bceaf785c12ec2a52215bea598fa30eed4f4c223</citedby><cites>FETCH-LOGICAL-c312t-cb0b538038fec6ea7f90ca749bceaf785c12ec2a52215bea598fa30eed4f4c223</cites><orcidid>0000-0002-3846-4279 ; 0000-0003-2880-9736 ; 0000-0003-1681-6330 ; 0000-0003-0517-7318 ; 0000-0002-6114-1996 ; 0000-0001-6384-8437</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://iopscience.iop.org/article/10.1088/1741-4326/ac95aa/pdf$$EPDF$$P50$$Giop$$H</linktopdf><link.rule.ids>314,776,780,27901,27902,53821,53868</link.rule.ids></links><search><creatorcontrib>Liu, B.</creatorcontrib><creatorcontrib>Dai, S.Y.</creatorcontrib><creatorcontrib>Yang, X.D.</creatorcontrib><creatorcontrib>Chan, V.S.</creatorcontrib><creatorcontrib>Ding, R.</creatorcontrib><creatorcontrib>Zhang, H.M.</creatorcontrib><creatorcontrib>Feng, Y.</creatorcontrib><creatorcontrib>Wang, D.Z.</creatorcontrib><title>Evaluation of edge transport and core accumulation of tungsten for CFETR with EMC3-EIRENE and STRAHL</title><title>Nuclear fusion</title><addtitle>NF</addtitle><addtitle>Nucl. Fusion</addtitle><description>The edge transport and core accumulation of tungsten (W) particles on China Fusion Engineering Test Reactor (CFETR) have been studied by integrated modelling consisting of EMC3-EIRENE and STRAHL codes. The edge transport and power dissipation of W particles are simulated by EMC3-EIRENE. An in–out asymmetry of W
(1–28)+
ions density has been revealed in the in- and out-board divertor regions. This is mainly due to the stronger reversal flow velocity of W ions at the outboard divertor. The upward flow of W ions near the separatrix leads to a moderate W impurity leakage from the divertor on CFETR compared to the existing full W device ASDEX Upgrade due to the high plasma density near the CFETR divertor targets. Further, the density distribution and radiation loss of W ions in the core region are investigated by STRAHL code. The high charge-state W
(29–60)+
and W
(61–74)+
ions mainly reside in the regions of Ψ
N
= 0.20–0.98 and 0.00–0.90 (Ψ
N
is the normalized poloidal magnetic flux), respectively. The W induced energy dissipation in different regions is assessed according to both STRAHL and EMC3-EIRENE simulations. Particularly, the impacts of the W core radiation on the operation regime are discussed according to the H-mode threshold scaling law proposed by Martin
et al
(2008
J. Phys.: Conf. Ser.
123
012033) for the baseline plasma on CFETR. Further, parameter studies on the pinch velocity (
v
imp
) and diffusion coefficient (
D
imp
) have been performed to check their impacts on the operation regime of CFETR. A three-fold increase of
v
imp
/
D
imp
results in a higher W core energy loss, which can lead to the transition from H-mode back to L-mode.</description><subject>CFETR</subject><subject>EMC3-EIRENE</subject><subject>STRAHL</subject><subject>tungsten distribution</subject><issn>0029-5515</issn><issn>1741-4326</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNp1kE1Lw0AQhhdRsFbvHvfmxdj9yObjKCHaQlWo9bxMNrs1pc2G3Y3ivzex0pPCwMDwPi_Dg9A1JXeUZNmMpjGNYs6SGahcAJygyfF0iiaEsDwSgopzdOH9lhAaU84nqC4_YNdDaGyLrcG63mgcHLS-sy5gaGusrNMYlOr3_e6YC3278UG32FiHi4dyvcKfTXjH5VPBo3KxKp_LH_h1vbqfLy_RmYGd11e_e4reBqSYR8uXx0Vxv4wUpyxEqiKV4BnhmdEq0ZCanChI47xSGkyaCUWZVgwEY1RUGkSeGeBE6zo2sWKMTxE59CpnvXfayM41e3BfkhI5WpKjEjkqkQdLA3JzQBrbya3tXTs8KFsjEybpOAmJiexqMyRv_0j-W_wNy_B1-g</recordid><startdate>20221201</startdate><enddate>20221201</enddate><creator>Liu, B.</creator><creator>Dai, S.Y.</creator><creator>Yang, X.D.</creator><creator>Chan, V.S.</creator><creator>Ding, R.</creator><creator>Zhang, H.M.</creator><creator>Feng, Y.</creator><creator>Wang, D.Z.</creator><general>IOP Publishing</general><scope>AAYXX</scope><scope>CITATION</scope><orcidid>https://orcid.org/0000-0002-3846-4279</orcidid><orcidid>https://orcid.org/0000-0003-2880-9736</orcidid><orcidid>https://orcid.org/0000-0003-1681-6330</orcidid><orcidid>https://orcid.org/0000-0003-0517-7318</orcidid><orcidid>https://orcid.org/0000-0002-6114-1996</orcidid><orcidid>https://orcid.org/0000-0001-6384-8437</orcidid></search><sort><creationdate>20221201</creationdate><title>Evaluation of edge transport and core accumulation of tungsten for CFETR with EMC3-EIRENE and STRAHL</title><author>Liu, B. ; Dai, S.Y. ; Yang, X.D. ; Chan, V.S. ; Ding, R. ; Zhang, H.M. ; Feng, Y. ; Wang, D.Z.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c312t-cb0b538038fec6ea7f90ca749bceaf785c12ec2a52215bea598fa30eed4f4c223</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>CFETR</topic><topic>EMC3-EIRENE</topic><topic>STRAHL</topic><topic>tungsten distribution</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Liu, B.</creatorcontrib><creatorcontrib>Dai, S.Y.</creatorcontrib><creatorcontrib>Yang, X.D.</creatorcontrib><creatorcontrib>Chan, V.S.</creatorcontrib><creatorcontrib>Ding, R.</creatorcontrib><creatorcontrib>Zhang, H.M.</creatorcontrib><creatorcontrib>Feng, Y.</creatorcontrib><creatorcontrib>Wang, D.Z.</creatorcontrib><collection>CrossRef</collection><jtitle>Nuclear fusion</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Liu, B.</au><au>Dai, S.Y.</au><au>Yang, X.D.</au><au>Chan, V.S.</au><au>Ding, R.</au><au>Zhang, H.M.</au><au>Feng, Y.</au><au>Wang, D.Z.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Evaluation of edge transport and core accumulation of tungsten for CFETR with EMC3-EIRENE and STRAHL</atitle><jtitle>Nuclear fusion</jtitle><stitle>NF</stitle><addtitle>Nucl. Fusion</addtitle><date>2022-12-01</date><risdate>2022</risdate><volume>62</volume><issue>12</issue><spage>126040</spage><pages>126040-</pages><issn>0029-5515</issn><eissn>1741-4326</eissn><coden>NUFUAU</coden><abstract>The edge transport and core accumulation of tungsten (W) particles on China Fusion Engineering Test Reactor (CFETR) have been studied by integrated modelling consisting of EMC3-EIRENE and STRAHL codes. The edge transport and power dissipation of W particles are simulated by EMC3-EIRENE. An in–out asymmetry of W
(1–28)+
ions density has been revealed in the in- and out-board divertor regions. This is mainly due to the stronger reversal flow velocity of W ions at the outboard divertor. The upward flow of W ions near the separatrix leads to a moderate W impurity leakage from the divertor on CFETR compared to the existing full W device ASDEX Upgrade due to the high plasma density near the CFETR divertor targets. Further, the density distribution and radiation loss of W ions in the core region are investigated by STRAHL code. The high charge-state W
(29–60)+
and W
(61–74)+
ions mainly reside in the regions of Ψ
N
= 0.20–0.98 and 0.00–0.90 (Ψ
N
is the normalized poloidal magnetic flux), respectively. The W induced energy dissipation in different regions is assessed according to both STRAHL and EMC3-EIRENE simulations. Particularly, the impacts of the W core radiation on the operation regime are discussed according to the H-mode threshold scaling law proposed by Martin
et al
(2008
J. Phys.: Conf. Ser.
123
012033) for the baseline plasma on CFETR. Further, parameter studies on the pinch velocity (
v
imp
) and diffusion coefficient (
D
imp
) have been performed to check their impacts on the operation regime of CFETR. A three-fold increase of
v
imp
/
D
imp
results in a higher W core energy loss, which can lead to the transition from H-mode back to L-mode.</abstract><pub>IOP Publishing</pub><doi>10.1088/1741-4326/ac95aa</doi><tpages>12</tpages><orcidid>https://orcid.org/0000-0002-3846-4279</orcidid><orcidid>https://orcid.org/0000-0003-2880-9736</orcidid><orcidid>https://orcid.org/0000-0003-1681-6330</orcidid><orcidid>https://orcid.org/0000-0003-0517-7318</orcidid><orcidid>https://orcid.org/0000-0002-6114-1996</orcidid><orcidid>https://orcid.org/0000-0001-6384-8437</orcidid></addata></record> |
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subjects | CFETR EMC3-EIRENE STRAHL tungsten distribution |
title | Evaluation of edge transport and core accumulation of tungsten for CFETR with EMC3-EIRENE and STRAHL |
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