2019
DOI: 10.1063/1.5124376
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Development and testing of an unstructured mesh method for whole plasma gyrokinetic simulations in realistic tokamak geometry

Abstract: In this work, we have formulated and implemented a mixed unstructured mesh-based finite element (FE)-Fourier decomposition scheme for gyrokinetic simulations in realistic tokamak geometry. An efficient particle positioning (particle-triangle mapping) scheme for the charge deposition and field scattering using an intermediate grid as the search index for triangles has been implemented and a significant speed-up by a factor of ∼ 30 is observed as compared with the brute force scheme for a medium-size simulation.… Show more

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Cited by 13 publications
(16 citation statements)
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“…The gyrokinetic codes are closest to first principles with the most important physics included, but re-quire long simulation times and consume significant amount of computing resources, especially when studying the nonlinear, multiple spatial and temporal scale physics [7,15,20]. A variety of codes made specific simplifications to achieve the balance between the computational cost and important physics.…”
Section: Simulation Models and Parametersmentioning
confidence: 99%
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“…The gyrokinetic codes are closest to first principles with the most important physics included, but re-quire long simulation times and consume significant amount of computing resources, especially when studying the nonlinear, multiple spatial and temporal scale physics [7,15,20]. A variety of codes made specific simplifications to achieve the balance between the computational cost and important physics.…”
Section: Simulation Models and Parametersmentioning
confidence: 99%
“…In the complex Gaussian expression A(s) = e −σ(s−s 0 ) 2 of radial envelope, the MSSB parameters σ and s 0 are obtained by fitting the radial mode structures simulated by the gyrokinetic eigenvalue code LIGKA [19], the initial value hybrid MHD-gyrokinetic code HMGC [17,18] and the full-f gyrokinetic code TRIMEG-GKX [15,16]. With the more consistent σ, s 0 as the input of HAGIS [6] code, the EP transport is studied.…”
Section: Physical Modelsmentioning
confidence: 99%
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“…2. a mixed implicit-explicit scheme for particle simulations, with analytical simplifications, as a practical way to upgrade the TRIMEG code 14 , meanwhile also as a potential solution for JOREK and other existing codes 4,15,16 , for dealing with full f electromagnetic simulations;…”
Section: Introductionmentioning
confidence: 99%