FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W4304588287> ?p ?o ?g. }

• W4304588287 endingPage "016017" @default.
• W4304588287 startingPage "016017" @default.
• W4304588287 abstract "Abstract Edge codes such as SOLPS coupled to neutral codes such as EIRENE have become so comprehensive and sophisticated that they now constitute, in effect, ‘code-experiments’ that, as for actual experiments, can benefit from interpretation using simple models and conceptual frameworks, i.e. reduced models. The first task is the identification of options for the reduced model control parameters that are best suited for control of the action of the divertor, i.e. for control of target power loading and sputter–erosion, primarily. A strong correlation between the electron temperature at the divertor target, T e,t , and the neutral deuterium D 2 density at the target, n D2,t , flux-tube resolved, has recently been reported for a number of code studies including SOLPS-4.3 modeling of a set of ∼50 ITER baseline cases: Q DT = 10, q 95 = 3, P SOL = 100 MW, metallic walls, and Ne seeding (Pitts et al 2019). Part A of the present study reports new results for largely the same ITER cases, confirming the strong correlation reported earlier between local values of T e,t , and (i) n D2,t , and (ii) normalized volumetric losses of power and pressure in the divertor. Strong correlations have now also been found, and are reported here for the first time, between T e,t and all of the divertor target quantities of practical interest. A physical explanation for this surprising result has not as yet been fully identified; nevertheless it has encouraging implications for reduced modeling of the ITER divertor. For such ITER conditions, (i) the global Ne injection rate, Inj Ne (Ne s −1 ), and (ii) the electron temperature at the location on the target where the peak power deposition occurs, T e,t @q ⊥,pk (eV), are found to be promising reduced model control parameters. In this part B, a reduced model for the ITER divertor is developed and described in detail, based on reversed-direction two point modeling, Rev2PM. The input to the reduced model is a value of the variable pair <?CDATA $left({T}_{text{e},mathrm{t}}@{q}_{perp ,mathrm{p}mathrm{k}},mathrm{I}mathrm{n}{mathrm{j}}_{text{Ne}}right)$?> <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline overflow=scroll> <mml:mfenced close=) open=(> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi>T</mml:mi> </mml:mrow> <mml:mrow> <mml:mtext>e</mml:mtext> <mml:mo>,</mml:mo> <mml:mi mathvariant=normal>t</mml:mi> </mml:mrow> </mml:msub> <mml:mi>@</mml:mi> <mml:msub> <mml:mrow> <mml:mi>q</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>⊥</mml:mo> <mml:mo>,</mml:mo> <mml:mi mathvariant=normal>p</mml:mi> <mml:mi mathvariant=normal>k</mml:mi> </mml:mrow> </mml:msub> <mml:mo>,</mml:mo> <mml:mi mathvariant=normal>I</mml:mi> <mml:mi mathvariant=normal>n</mml:mi> <mml:msub> <mml:mrow> <mml:mi mathvariant=normal>j</mml:mi> </mml:mrow> <mml:mrow> <mml:mtext>Ne</mml:mtext> </mml:mrow> </mml:msub> </mml:mrow> </mml:mfenced> </mml:math> for a chosen case and the output are values of the various target as well as divertor-entrance quantities of practical interest, e.g. q ⊥,pk , the electron density at the X-point, n e,Xpt , etc. The reduced model was quantitatively characterized using one half of the code cases; it was then used to successfully predict (replicate) the code values of e.g. n e,Xpt for the other half." @default.
• W4304588287 created "2022-10-12" @default.
• W4304588287 creator A5007934502 @default.
• W4304588287 creator A5025421447 @default.
• W4304588287 creator A5033039391 @default.
• W4304588287 creator A5043388540 @default.
• W4304588287 creator A5056155860 @default.
• W4304588287 date "2022-12-13" @default.
• W4304588287 modified "2023-09-25" @default.
• W4304588287 title "A reduced model for the ITER divertor based on SOLPS solutions for ITER Q = 10 baseline conditions: B. A reduced model based on reversed-direction two point modeling ^*" @default.
• W4304588287 cites W2036360347 @default.
• W4304588287 cites W2791819631 @default.
• W4304588287 cites W2960401979 @default.
• W4304588287 cites W2982474733 @default.
• W4304588287 cites W2982641339 @default.
• W4304588287 cites W3128591958 @default.
• W4304588287 doi "https://doi.org/10.1088/1741-4326/ac9917" @default.
• W4304588287 hasPublicationYear "2022" @default.
• W4304588287 type Work @default.
• W4304588287 citedByCount "0" @default.
• W4304588287 crossrefType "journal-article" @default.
• W4304588287 hasAuthorship W4304588287A5007934502 @default.
• W4304588287 hasAuthorship W4304588287A5025421447 @default.
• W4304588287 hasAuthorship W4304588287A5033039391 @default.
• W4304588287 hasAuthorship W4304588287A5043388540 @default.
• W4304588287 hasAuthorship W4304588287A5056155860 @default.
• W4304588287 hasBestOaLocation W43045882871 @default.
• W4304588287 hasConcept C116515362 @default.
• W4304588287 hasConcept C116915560 @default.
• W4304588287 hasConcept C121332964 @default.
• W4304588287 hasConcept C127413603 @default.
• W4304588287 hasConcept C185544564 @default.
• W4304588287 hasConcept C2777017188 @default.
• W4304588287 hasConcept C82706917 @default.
• W4304588287 hasConceptScore W4304588287C116515362 @default.
• W4304588287 hasConceptScore W4304588287C116915560 @default.
• W4304588287 hasConceptScore W4304588287C121332964 @default.
• W4304588287 hasConceptScore W4304588287C127413603 @default.
• W4304588287 hasConceptScore W4304588287C185544564 @default.
• W4304588287 hasConceptScore W4304588287C2777017188 @default.
• W4304588287 hasConceptScore W4304588287C82706917 @default.
• W4304588287 hasIssue "1" @default.
• W4304588287 hasLocation W43045882871 @default.
• W4304588287 hasOpenAccess W4304588287 @default.
• W4304588287 hasPrimaryLocation W43045882871 @default.
• W4304588287 hasRelatedWork W2018971086 @default.
• W4304588287 hasRelatedWork W2022467141 @default.
• W4304588287 hasRelatedWork W2214421488 @default.
• W4304588287 hasRelatedWork W2227298166 @default.
• W4304588287 hasRelatedWork W2382181381 @default.
• W4304588287 hasRelatedWork W3128295357 @default.
• W4304588287 hasRelatedWork W3134396064 @default.
• W4304588287 hasRelatedWork W4200231759 @default.
• W4304588287 hasRelatedWork W4241039598 @default.
• W4304588287 hasRelatedWork W1981393467 @default.
• W4304588287 hasVolume "63" @default.
• W4304588287 isParatext "false" @default.
• W4304588287 isRetracted "false" @default.
• W4304588287 workType "article" @default.