Transcript
Page 1: Transport Code (   Thoughts, actions for                          use of, linkage to PDB)

Transport Code( Thoughts, actions for

use of, linkage to PDB)

M.Yokoyama

Page 2: Transport Code (   Thoughts, actions for                          use of, linkage to PDB)
Page 3: Transport Code (   Thoughts, actions for                          use of, linkage to PDB)

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)

Page 4: Transport Code (   Thoughts, actions for                          use of, linkage to PDB)

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 Rax,vac=3.75m, 3.60m NNW wrt <>, covering wide range of values

Page 5: Transport Code (   Thoughts, actions for                          use of, linkage to PDB)

Extension towards low-collisionality, finite (training data for NNW)

10-5

10-3

10-1

101

103

105

107

10-8 10-6 10-4 10-2 100 102

r375q100b298a8020.rho050

0.00E+001.00E-033.16E-031.00E-023.16E-021.00E-01GSRAKE

D*

*

10-5

10-3

10-1

101

103

105

107

10-8 10-6 10-4 10-2 100 102

r375q100b199a8020.rho050

0.00E+001.00E-033.16E-031.00E-023.16E-021.00E-01GSRAKE

D*

*

10-5

10-3

10-1

101

103

105

107

10-8 10-6 10-4 10-2 100 102

r375q100b100a8020.rho050

0.00E+001.00E-033.16E-031.00E-023.16E-021.00E-01GSRAKE

D*

*

Rax,vac=3.75m, =0.5

b100 (~1%)

b298 (~3%)b199 (~2%)

•D* agrees in this range of •D* agrees in this range of

Page 6: Transport Code (   Thoughts, actions for                          use of, linkage to PDB)

Extension towards low-collisionality, finite (training data for NNW)

Rax,vac=3.75m, =0.9

b100 (~1%)

b298 (~3%)b199 (~2%)

10-5

10-3

10-1

101

103

105

107

10-8 10-6 10-4 10-2 100 102

r375q100b100a8020.rho090

0.00E+001.00E-03

1.00E-02

1.00E-01GSRAKE

D*

*

10-5

10-3

10-1

101

103

105

107

10-8 10-6 10-4 10-2 100 102

r375q100b199a8020.rho090

0.00E+001.00E-033.16E-031.00E-023.16E-021.00E-01GSRAKE

D*

*

10-5

10-3

10-1

101

103

105

107

10-8 10-6 10-4 10-2 100 102

r375q100b298a8020.rho090

0.00E+001.00E-033.16E-031.00E-023.16E-021.00E-01GSRAKE

D*

*

•D*@Er=0 becomes to differ as is increased (smaller in GSRAKE, limited Bmns)

•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 Bmns)

•However, D* at finite Er agrees well (can be “practically” applicable to experimental analysis)

Page 7: Transport Code (   Thoughts, actions for                          use of, linkage to PDB)

(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 DBIPP (W7-AS,X): DKESNIFS (LHD): DGN/LHDOthers: ???

M.Sato Y.Turkin D.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

Page 8: Transport Code (   Thoughts, actions for                          use of, linkage to PDB)

ISH-PDB: providing equilibria to codes (users)

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 .bcSPBSC (Boozer)

MHDCAS3D, TERPSICHORE,,,•CAS3D: VMEC•TERPSICHORE: VMEC

Edge physicsEMC3/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&CDTRAVIS, TRECE,,,•TRAVIS: Boozer•TRECE:

Integrated/Predictive transport codesTASK/3D, IPP, ASTRA,,,•VMEC calu. frequently, or, using equilibrium DB ?

Page 9: Transport Code (   Thoughts, actions for                          use of, linkage to PDB)

b0=1%

b0=2%b0=3%

Rax=3.60 mr/a = 0.5

Page 10: Transport Code (   Thoughts, actions for                          use of, linkage to PDB)

Rax=3.60 mr/a = 0.9 b0=1%

b0=2%b0=3%