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Transport Code (  Thoughts, actions for use of, linkage to PDB) M.Yokoyama.

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Presentation on theme: "Transport Code (  Thoughts, actions for use of, linkage to PDB) M.Yokoyama."— Presentation transcript:

1 Transport Code (  Thoughts, actions for use of, linkage to PDB) M.Yokoyama

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3 On Use of PDB (by transport codes) Compatibility (readability) of 2D Ufiles checked by TASK3D(Sato), IPP (Turkin) and ASTRA (Estrada) (Apr. 09) NC database for transport module (specific-physics in helical systems: particularly important for transport analysis) Extension of DCOM/NNW : vacuum to finite beta, lower collisionality (Wakasa, Yokoyama) Equilibrium Data equilibrium information corresponding to registered shots Some examples for W7-AS high-beta shots: 54022, 54023 (Geiger) triggering comments/demands/usability investigation ! (boost the discussions) inputs from LHD high-beta talks (this afternoon)

4 NC database for NC module We should equip NC DB to be applicable to (at least) registered shots Moreover, DB covering a wide range of parameters are required Certainly not enough at one specific radius DCOM/NNW has been one of attempts to deliver NC DB to transport codes (A.Wakasa et al., JJAP 46 (2007) 1157.) It has been extended to Lower collisionality (where Monte-Carlo gets so time-consuming) (M.Yokoyama)  Increased accuracy of NNW (DGN/LHD, ITC18(2008)) to be applicable to low-collisional plasmas (eg., CERC) finite beta equilibrium (utilizing the LHD VMEC-DB) (A.Wakasa) ~ 1, 2, 3 % of R ax,vac =3.75m, 3.60m  NNW wrt, covering wide range of  values

5 Extension towards low-collisionality, finite  (training data for NNW) Rax,vac=3.75m,  =0.5 b100 (~1%) b298 (~3%)b199 (~2%) D* agrees in this range of 

6 Extension towards low-collisionality, finite  (training data for NNW) Rax,vac=3.75m,  =0.9 b100 (~1%) b298 (~3%)b199 (~2%) D*@Er=0 becomes to differ as  is increased (smaller in GSRAKE, limited B mn s) However, D* at finite Er agrees well (can be “practically” applicable to experimental analysis) D*@Er=0 becomes to differ as  is increased (smaller in GSRAKE, limited B mn s) However, D* at finite Er agrees well (can be “practically” applicable to experimental analysis)

7 (Modified) Transport Codes Session (CWGM4, Oct.2008) TASK/3D (NIFS) Heating NC ambEr Anomalous model IPP Heating NC ambEr Anomalous model ASTRA (CIEMAT) Heating NC ambEr Anomalous model Benchmarking on NC NC DB IPP (W7-AS,X): DKES NIFS (LHD): DGN/LHD Others: ??? M.SatoY.TurkinD.Lopez-Bruna Convolution for NC flux estimate Ambipolar Er determination PDB Test bed for physics benchmarking 2D Ufiles Interface to mutual DB (Sato) 2D Ufiles : accessible equilibrium Examples provided Try them: whether they are enough or not ? Benchmarking on MHD, GK

8 ISH-PDB: providing equilibria to codes (users) ISH-PDB Profile (fitting coeff. fitting function) Equilibria : (VMEC2000: netCDF ver, wout, fort.8) (cf., J.Geiger’s presentation) Neoclassical transport (ICNTS) DKES, DCOM, MOCA, GSRAKE, NEO(2), VENUS-δf, PENTA,,, Boozer equilibria (.bc,.newboz, etc…) stored in a common directory interface fully equipped .bc SPBSC (Boozer) MHD CAS3D, TERPSICHORE,,, CAS3D: VMEC TERPSICHORE: VMEC Edge physics EMC3/EIRENE,DEGAS,,, EIRENE: B on (R,φ,Z): field-line trace, HINT(2) Energetic particles GNET, DELTA5D,,, GNET: Boozer (NEWBOZ: NIFS-Kyoto) DELTA5D: Boozer (XBOZ; Spong)  Adapting interface of ICNTS activity Turbulent transport GKV, GENE, GS2, GOBLIN,,, GKV: currently picked up from VMEC out (radial derivative required for global flux tube sim., later on) GS2: VMEC out->TERPSICHORE (Boozer)->VVBAL (geometry in balloon. coor.) -> GS2 Proposal: Survey of possible users (codes) requests from users on equilibria Assurance of accuracy, consensus required Successful achievement through DB  feedback  “defacto standard” Heating&CD TRAVIS, TRECE,,, TRAVIS: Boozer TRECE: Integrated/Predictive transport codes TASK/3D, IPP, ASTRA,,, VMEC calu. frequently, or, using equilibrium DB ?

9 b 0 =1% b 0 =2% b 0 =3% Rax=3.60 m r/a = 0.5

10 Rax=3.60 m r/a = 0.9 b 0 =1% b 0 =2% b 0 =3%


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