2022
DOI: 10.1088/1361-6587/ac4fac
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Implementation of multi-component Zhdanov closure in SOLEDGE3X

Abstract: The multi-component fluid closure derived by Zhdanov is implemented in the fluid code SOLEDGE3X-EIRENE to deal with arbitrary edge plasma composition. The closure assumes no distinction in between species such as light vs heavy species separation. The work of Zhdanov is rewritten in a matrix form in order to clearly link friction forces and heat fluxes to the different species velocities and temperature gradients.

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Cited by 19 publications
(17 citation statements)
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“…The species temperature T is used to compute species pressure p = nT and species total energy E = 3 2 nT + 1 2 mnv 2 . Parallel viscosity ν , parallel heat conductivity κ , parallel friction force in between species R , parallel heat flux due to inter-species collisions h and energy equipartition term Q take values computed by Zhdanov collisional closure for multi-component plasmas [5,9,10,11]. For a simple hydrogenic plasma, Braginskiis closure can also be used.…”
Section: The Drift-fluid Model Implemented In Soledge3xmentioning
confidence: 99%
See 1 more Smart Citation
“…The species temperature T is used to compute species pressure p = nT and species total energy E = 3 2 nT + 1 2 mnv 2 . Parallel viscosity ν , parallel heat conductivity κ , parallel friction force in between species R , parallel heat flux due to inter-species collisions h and energy equipartition term Q take values computed by Zhdanov collisional closure for multi-component plasmas [5,9,10,11]. For a simple hydrogenic plasma, Braginskiis closure can also be used.…”
Section: The Drift-fluid Model Implemented In Soledge3xmentioning
confidence: 99%
“…The implementation of the different operators has been verified using the method of manufactured solution [11].…”
Section: Numerical Implementationmentioning
confidence: 99%
“…[5] This is important for modelling impurity dynamics because impurities may be present as a significant fraction of the background plasma species, or, in case of deuterium-tritium plasmas, tritium, being a main ion species, cannot be modelled as trace over an existing deuterium-electron plasma. The Zhdanov closure is already implemented, though only using single-temperature collision coefficients at the plasma common temperature, in SOL/edge simulators such as Soledge3x-EIRENE, [1,6,7] SOLPS, [8][9][10] B2-EIRENE, [11] and EDGE2D. [12] Generally, the depth of the closure is represented by the number of moments, that is, 5N-moment, 13N-moment, 21N-moment, or 29N-moment, where N represents the number of species.…”
Section: Introductionmentioning
confidence: 99%
“…[3] For example, this method can be used for deuterium and tritium mixture simulations in future and present machines. [5] It is important to mention that multi-temperature generalization of this method is in progress for the SOLEDGE3X-EIRENE code. [6,7] In the present paper, a new Grad-Zhdanov module based on the improved approach [8] and complete Grad-Zhdanov method [3,8] has been implemented in the SOLPS-ITER code (Section 2).…”
Section: Introductionmentioning
confidence: 99%