Parallel flows as a key component to interpret Super-X divertor experiments Article Swipe
M. Carpita
,
O. Février
,
H. Reimerdes
,
C. Theiler
,
B.P. Duval
,
C. Colandrea
,
G. Durr-Legoupil-Nicoud
,
D. Galassi
,
S. Gorno
,
E. Huett
,
J. Loizu
,
L. Martinelli
,
A. Perek
,
L. Simons
,
Guangyu Sun
,
E. Tonello
,
C. Wüthrich
·
YOU?
·
· 2024
· Open Access
·
· DOI: https://doi.org/10.1088/1741-4326/ad2a2a
YOU?
·
· 2024
· Open Access
·
· DOI: https://doi.org/10.1088/1741-4326/ad2a2a
The Super-X Divertor (SXD) is an alternative divertor configuration leveraging total flux expansion at the Outer Strike Point (OSP). While the extended 2-Point Model (2PM) predicts facilitated detachment access and control in the SXD configuration, these attractive features are not always retrieved experimentally. These discrepancies are at least partially explained by the effect of parallel flows which, when self-consistently included in the 2PM, reveal the role of total flux expansion on the pressure balance and weaken the total flux expansion effect on detachment access and control, compared to the original predictions. This new model can partially explain the discrepancies between the 2PM and experiments performed on tokamak à configuration variable (TCV), in ohmic L-mode scenarios, which are particularly apparent when scanning the OSP major radius Rt. In core density ramps in lower Single-Null (SN) configuration, the impact of Rt on the CIII emission front movement in the divertor outer leg—used as a proxy for the plasma temperature in the divertor—is substantially weaker than 2PM predictions. Furthermore, in OSP radial sweeps in lower and upper SN configurations, in ohmic L-mode scenarios with a constant core density, the peak parallel particle flux density at the OSP is almost independent of Rt, while the 2PM predicts a linear dependence. Finally, analytical and numerical modeling of parallel flows in the divertor is presented. It is shown that an increase in total flux expansion can favour supersonic flows at the OSP. Parallel flows are also shown to be relevant by analysing SOLPS-ITER simulations of TCV.
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- Type
- article
- Language
- en
- Landing Page
- https://doi.org/10.1088/1741-4326/ad2a2a
- https://iopscience.iop.org/article/10.1088/1741-4326/ad2a2a/pdf
- OA Status
- diamond
- Cited By
- 5
- References
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- Related Works
- 10
- OpenAlex ID
- https://openalex.org/W4391874397
All OpenAlex metadata
Raw OpenAlex JSON
- OpenAlex ID
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https://openalex.org/W4391874397Canonical identifier for this work in OpenAlex
- DOI
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https://doi.org/10.1088/1741-4326/ad2a2aDigital Object Identifier
- Title
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Parallel flows as a key component to interpret Super-X divertor experimentsWork title
- Type
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articleOpenAlex work type
- Language
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enPrimary language
- Publication year
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2024Year of publication
- Publication date
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2024-02-16Full publication date if available
- Authors
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M. Carpita, O. Février, H. Reimerdes, C. Theiler, B.P. Duval, C. Colandrea, G. Durr-Legoupil-Nicoud, D. Galassi, S. Gorno, E. Huett, J. Loizu, L. Martinelli, A. Perek, L. Simons, Guangyu Sun, E. Tonello, C. WüthrichList of authors in order
- Landing page
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https://doi.org/10.1088/1741-4326/ad2a2aPublisher landing page
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https://iopscience.iop.org/article/10.1088/1741-4326/ad2a2a/pdfDirect link to full text PDF
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YesWhether a free full text is available
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diamondOpen access status per OpenAlex
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https://iopscience.iop.org/article/10.1088/1741-4326/ad2a2a/pdfDirect OA link when available
- Concepts
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Divertor, Plasma, Mechanics, Physics, RADIUS, Tokamak, Flux (metallurgy), Supersonic speed, Computational physics, Atomic physics, Materials science, Nuclear physics, Computer security, Metallurgy, Computer scienceTop concepts (fields/topics) attached by OpenAlex
- Cited by
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5Total citation count in OpenAlex
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2025: 2, 2024: 3Per-year citation counts (last 5 years)
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41Number of works referenced by this work
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10Other works algorithmically related by OpenAlex
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| abstract_inverted_index.peak | 187 |
| abstract_inverted_index.role | 66 |
| abstract_inverted_index.than | 163 |
| abstract_inverted_index.that | 223 |
| abstract_inverted_index.when | 58, 120 |
| abstract_inverted_index.with | 181 |
| abstract_inverted_index.(2PM) | 25 |
| abstract_inverted_index.(SXD) | 4 |
| abstract_inverted_index.Model | 24 |
| abstract_inverted_index.Outer | 16 |
| abstract_inverted_index.Point | 18 |
| abstract_inverted_index.These | 44 |
| abstract_inverted_index.While | 20 |
| abstract_inverted_index.flows | 56, 214, 233, 238 |
| abstract_inverted_index.front | 144 |
| abstract_inverted_index.least | 48 |
| abstract_inverted_index.lower | 132, 172 |
| abstract_inverted_index.major | 124 |
| abstract_inverted_index.model | 94 |
| abstract_inverted_index.ohmic | 113, 178 |
| abstract_inverted_index.outer | 149 |
| abstract_inverted_index.proxy | 153 |
| abstract_inverted_index.ramps | 130 |
| abstract_inverted_index.shown | 222, 241 |
| abstract_inverted_index.these | 36 |
| abstract_inverted_index.total | 11, 68, 78, 227 |
| abstract_inverted_index.upper | 174 |
| abstract_inverted_index.which | 116 |
| abstract_inverted_index.while | 200 |
| abstract_inverted_index.(OSP). | 19 |
| abstract_inverted_index.(TCV), | 111 |
| abstract_inverted_index.L-mode | 114, 179 |
| abstract_inverted_index.Strike | 17 |
| abstract_inverted_index.access | 29, 84 |
| abstract_inverted_index.almost | 196 |
| abstract_inverted_index.always | 41 |
| abstract_inverted_index.effect | 53, 81 |
| abstract_inverted_index.favour | 231 |
| abstract_inverted_index.impact | 137 |
| abstract_inverted_index.linear | 205 |
| abstract_inverted_index.plasma | 156 |
| abstract_inverted_index.radial | 169 |
| abstract_inverted_index.radius | 125 |
| abstract_inverted_index.reveal | 64 |
| abstract_inverted_index.sweeps | 170 |
| abstract_inverted_index.weaken | 76 |
| abstract_inverted_index.weaker | 162 |
| abstract_inverted_index.which, | 57 |
| abstract_inverted_index.2-Point | 23 |
| abstract_inverted_index.Super-X | 2 |
| abstract_inverted_index.balance | 74 |
| abstract_inverted_index.between | 100 |
| abstract_inverted_index.control | 31 |
| abstract_inverted_index.density | 129, 191 |
| abstract_inverted_index.explain | 97 |
| abstract_inverted_index.tokamak | 107 |
| abstract_inverted_index.Abstract | 0 |
| abstract_inverted_index.Divertor | 3 |
| abstract_inverted_index.Finally, | 207 |
| abstract_inverted_index.Parallel | 237 |
| abstract_inverted_index.apparent | 119 |
| abstract_inverted_index.compared | 87 |
| abstract_inverted_index.constant | 183 |
| abstract_inverted_index.control, | 86 |
| abstract_inverted_index.density, | 185 |
| abstract_inverted_index.divertor | 8, 148, 217 |
| abstract_inverted_index.emission | 143 |
| abstract_inverted_index.extended | 22 |
| abstract_inverted_index.features | 38 |
| abstract_inverted_index.included | 60 |
| abstract_inverted_index.increase | 225 |
| abstract_inverted_index.modeling | 211 |
| abstract_inverted_index.movement | 145 |
| abstract_inverted_index.original | 90 |
| abstract_inverted_index.parallel | 55, 188, 213 |
| abstract_inverted_index.particle | 189 |
| abstract_inverted_index.predicts | 26, 203 |
| abstract_inverted_index.pressure | 73 |
| abstract_inverted_index.relevant | 244 |
| abstract_inverted_index.scanning | 121 |
| abstract_inverted_index.variable | 110 |
| abstract_inverted_index.analysing | 246 |
| abstract_inverted_index.expansion | 13, 70, 80, 229 |
| abstract_inverted_index.explained | 50 |
| abstract_inverted_index.numerical | 210 |
| abstract_inverted_index.partially | 49, 96 |
| abstract_inverted_index.performed | 105 |
| abstract_inverted_index.retrieved | 42 |
| abstract_inverted_index.scenarios | 180 |
| abstract_inverted_index.SOLPS-ITER | 247 |
| abstract_inverted_index.analytical | 208 |
| abstract_inverted_index.attractive | 37 |
| abstract_inverted_index.detachment | 28, 83 |
| abstract_inverted_index.leg—used | 150 |
| abstract_inverted_index.leveraging | 10 |
| abstract_inverted_index.presented. | 219 |
| abstract_inverted_index.scenarios, | 115 |
| abstract_inverted_index.supersonic | 232 |
| abstract_inverted_index.Single-Null | 133 |
| abstract_inverted_index.alternative | 7 |
| abstract_inverted_index.dependence. | 206 |
| abstract_inverted_index.experiments | 104 |
| abstract_inverted_index.facilitated | 27 |
| abstract_inverted_index.independent | 197 |
| abstract_inverted_index.simulations | 248 |
| abstract_inverted_index.temperature | 157 |
| abstract_inverted_index.Furthermore, | 166 |
| abstract_inverted_index.particularly | 118 |
| abstract_inverted_index.predictions. | 91, 165 |
| abstract_inverted_index.configuration | 9, 109 |
| abstract_inverted_index.discrepancies | 45, 99 |
| abstract_inverted_index.divertor—is | 160 |
| abstract_inverted_index.substantially | 161 |
| abstract_inverted_index.configuration, | 35, 135 |
| abstract_inverted_index.configurations, | 176 |
| abstract_inverted_index.experimentally. | 43 |
| abstract_inverted_index.self-consistently | 59 |
| cited_by_percentile_year.max | 97 |
| cited_by_percentile_year.min | 95 |
| corresponding_author_ids | https://openalex.org/A5058322696 |
| countries_distinct_count | 3 |
| institutions_distinct_count | 17 |
| corresponding_institution_ids | https://openalex.org/I5124864 |
| citation_normalized_percentile.value | 0.95003267 |
| citation_normalized_percentile.is_in_top_1_percent | False |
| citation_normalized_percentile.is_in_top_10_percent | True |