Recent Progress in Integrate Code TASK

Transcription

1 US-Japan JIFT Workshop on Integrated Modeling on Fusion Plasmas ORNL, Oak Ridge, USA 2007/01/29 Recent Progress in Integrate Code TASK Integrated Modeling of RF Heating and Current Drive in Tokamaks A. Fukuyama Department of Nuclear Engineering, Kyoto University in collaboration with S. Murakami, M. Honda, A. Sonoda, T. Yamamoto

2 Outline Integrated Simulation of Fusion Plasmas Progress of TASK Code Development Self-Consistent Analysis of RF Heating and Current Drive Full Wave Analysis Including FLR Effects Future Plan of Integrated Modeling Summary

3 Burning Plasma Simulation Broad time scale: 100GHz 1000s Energetic Ion Confinement Broad Spatial scale: 10 μm 10m Transport Barrier MHD Stability Core Transport Non-Inductive CD EC LH IC MHD Turbulent Transport Impurity Transport SOL Transport RF Heating NBI Heating Neutral Transport Divertor Plasma Plasma-Wall Int. One simulation code never covers all range. Blanket, Neutronics, Tritium, Material, Heat and Fluid Flow Integrated simulation combining modeling codes interacting each other

4 Integrated Tokamak Simulation Integrated Simulation Equilibrium: Magnetic Island Diagnostic model Control model Anisotropic Pressure Fixed boundary Free boundary Time evolution Core Plasma Transport: Neoclassical Tranport Turbulent Tranport Neutral Transport Impurity Transport Energetic Particles Diffusive transport Dynamic transport Kinetic transport Orbit following Macroscopic Stability: Plasma Deformation MHD stability Kinetic stability Wave Heating Current Drive: Ray/Beam tracing Wave Despersion Velocity Distribut. Fn Full wave Peripheral Plasma Transport: Turbulent Transport Plasma-Wall Interaction Neutral Transport Impurity Transport Radiation Transport Fluid transport Kinetic transport

5 Multi-Hierarchy and Integrated Approaches Multi-Hierarchu Simulation Integrated Simulation Diagnostic model Control model Device size Nonlinear Equilibrium: Magnetic Island Anisotropic Pressure MHD Simulation Magnetic island size Core Plasma Transport: Ion gyroradius Extended MHD Simulation Neoclassical Tranport Turbulent Tranport Neutral Transport Impurity Transport Collsionless skin depth Energetic Particles Debye length Turbulence Simulation Macroscopic Stability: Plasma Deformation Electron gyroradius Particle distance Molecular Dynamics Wave Heating Current Drive: Wave Despersion Velocity Distribut. Fn Peripheral Plasma Transport: Turbulent Transport Plasma-Wall Interaction Neutral Transport Impurity Transport Radiation Transport

6 BPSI: Burning Plasma Simulation Initiative Integrated code: TASK and TOPICS

7 TASK Code Transport Analysing System for TokamaK Features Core of Integrated Modeling Code in BPSI Modular structure Reference data interface and standard data set Uniform user interface Various Heating and Current Drive Scheme High Portability Development using CVS (Concurrent Version System) Open Source: Parallel Processing using MPI Library Extension to Toroidal Helical Plasmas

8 Recent Progress of TASK Fortran95 TASK V1.0: Fortran95 compiler required (g95, pgf95, xlf95, ifort,...) TASK/EQ, TASK/TR: Fortran95 (Module, Dynamic allocation) Module structure Standard dataset: partially implemented Data exchange interface: prototype Execution control interface: prototype New module: fromtopicsby M. Azumi TOPICS/EQU: Free boundary 2D equilibrium TOPICS/NBI: Beam deposition + 1D Fokker-Planck MHD stability component: coming Self-consistent wave analysis Dynamic transport analysis: by M. Honda

9 Modules of TASK EQ 2D Equilibrium Fixed/Free boundary, Toroidal rotation TR 1D Transport Diffusive transport, Transport models WR 3D Geometr. Optics EC, LH: Ray tracing, Beam tracing WM 3D Full Wave IC, AW: Antenna excitation, Eigenmode FP 3D Fokker-Planck Relativistic, Bounce-averaged DP Wave Dispersion Local dielectric tensor, Arbitrary f (u) PL Data Interface Data conversion, Profile database LIB Libraries LIB, MTX, MPI Under Development TX Transport analysis including plasma rotation and E r Collaboration with TOPICS EQU Free boundary equilibrium NBI NBI heating

10 Structure of TASK

11 Inter-Module Collaboration Interface: TASK/PL Role of Module Interface Data exchange between modules: Standard dataset: Specify set of data (cf. ITPA profile DB) Specification of data exchange interface: initialize, set, get Execution control: Specification of execution control interface: initialize, setup, exec, visualize, terminate Uniform user interface: parameter input, graphic output Role of data exchange interface: TASK/PL Keep present status of plasma and device Store history of plasma Save into fileandloadfromfile Interface to experimental data base

12 Standard Dataset (interim) Shot data Machine ID, Shot ID, Model ID Device data: (Level1) RR R m Geometrical major radius RA a m Geometrical minor radius RB b m Wall radius BB B T Vacuum toroidal mag. field RKAP κ Elongation at boundary RDLT δ Triangularity at boundary RIP I p A Typical plasma current Equilibrium data: (Level1) PSI2D ψ p (R, Z) Tm 2 2D poloidal magnetic flux PSIT ψ t (ρ) Tm 2 Toroidal magnetic flux PSIP ψ p (ρ) Tm 2 Poloidal magnetic flux ITPSI I t (ρ) Tm Poloidal current: 2πB φ R IPPSI I p (ρ) Tm Toroidal current PPSI p(ρ) MPa Plasma pressure QINV 1/q(ρ) Inverse of safety factor Metric data 1D: V (ρ), V (ρ), 2D: g ij, 3D: g ij, Fluid plasma data NSMAX s Number of particle species PA A s Atomic mass PZ0 Z 0s Charge number PZ Z s Charge state number PN n s (ρ) m 3 Number density PT T s (ρ) ev Temperature PU u sφ (ρ) m/s Toroidal rotation velocity QINV 1/q(ρ) Inverse of safety factor Kinetic plasma data FP f (p,θ p,ρ) momentum dist. fn at θ = 0 Dielectric tensor data CEPS ɛ (ρ, χ, ζ) Local dielectric tensor Full wave field data CE E(ρ, χ, ζ)v/m Complex wave electric field CB B(ρ, χ, ζ)wb/m 2 Complex wave magnetic field Ray/Beam tracing field data RRAY R(l) m R of ray at length l ZRAY Z(l) m Z of ray at length l PRAY φ(l) rad φ of ray at length l CERAY E(l) V/m Wave electric field at length l PWRAY P(l) W Wave power at length l DRAY d(l) m Beam radius at length l VRAY u(l) 1/m Beam curvature at length l

13 Data Exchange Interface Data structure: Derived type (Fortran95): structured type time plasmaf%time number of grid plasmaf%nrmax e.g. square of grid radius plasmaf%s(nr) plasma density plasmaf%data(nr)%pn plasma temperature plasmaf%data(nr)%pt Program interface e.g. Initialize bpsd init data(ierr) Set data bpsd set data( plasmaf,plasmaf,ierr) Get data bpsd get data( plasmaf,plasmaf,ierr) Other functions: Save data into a file, Load data from a file, Plot data

14 Execution Control Interface Example for TASK/TR TR INIT Initialization (Default value) BPSX INIT( TR ) TR PARM(ID,PSTR) Parameter setup (Namelist input) BPSX PARM( TR,ID,PSTR) TR SETUP(T) Profile setup (Spatial profile, Time) BPSX SETUP( TR,T) TR EXEC(DT) Exec one step (Time step) BPSX EXEC( TR,DT) TR GOUT(PSTR) Plot data (Plot command) BPSX GOUT( TR,PSTR) TR SAVE Save data in file BPSX SAVE( TR ) TR LOAD load data from file BPSX LOAD( TR ) TR TERM Termination BPSX TERM( TR ) Module registration TR STRUCT%INIT=TR INIT TR STRUCT%PARM=TR PARM TR STRUCT%EXEC=TR EXEC BPSX REGISTER( TR,TR STRUCT)

15 Example of data structure: plasmaf type bpsd_plasmaf_data real(8) :: pn! Number density [mˆ-3] real(8) :: pt! Temperature [ev] real(8) :: ptpr! Parallel temperature [ev] real(8) :: ptpp! Perpendicular temperature [ev] real(8) :: pu! Parallel flow velocity [m/s] end type bpsd_plasmaf_data type bpsd_plasmaf_type real(8) :: time integer :: nrmax! Number of radial points integer :: nsmax! Number of particle species real(8), dimension(:), allocatable :: s! (rhoˆ2) : normarized toroidal flux real(8), dimension(:), allocatable :: qinv! 1/q : inverse of safety factor type(bpsd_plasmaf_data), dimension(:,:), allocatable :: data end type bpsd_plasmaf_type

16 Examples of sequence in a module TR EXEC(dt) call bpsd get data( plasmaf,plasmaf,ierr) call bpsd get data( metric1d,metric1d,ierr) local data <- plasmaf,metric1d advance time step dt plasmaf <- local data call bpsd set data( plasmaf,plasmaf,ierr) EQ CALC call bpsd get data( plasmaf,plasmaf,ierr) local data <- plasmaf calculate equilibrium update plasmaf call bpsd set data( plasmaf,plasmaf,ierr) equ1d,metric1d <- local data call bpsd set data( equ1d,equ1d,ierr) call bpsd set data( metric1d,metric1d,ierr)

17 Example: Coupling of TASK/TR and TOPICS/EQU TOPICS/EQU: Free boundary 2D equilibrium TASK/TR Diffusive 1D transport (CDBM + Neoclassical) QUEST parameters: R = 0.64 m, a = 036 m, B = 0.64 T, I p = 300 ka, OH+LHCD ψ p (R, Z) j φ T e (ρ, t) j (ρ, t) psi(r,z) rcu(r,z) TE [kev] vs t AJ [A/m^2] vs t

18 Transport simulation OH + off-axis LHCD: 200 kw Formation of internal transport barrier (equilibrium not solved) PIN,POH,PNB,PRF,PNF,PEX [MW] vs t P OH P TOT P LH WF,WB,WI,WE [MJ] vs t W tot W e TE,TD,<TE>,<TD> [kev] vs t T e (0) T i (0) IPPRL,IOH,INB,IRF,IBS,IP [MA] vs t I OH ILH I BS TE,TD [kev] vs r T e T i AKD,AKNCD,AKDWD [m 2 /s] vs r χ i χ TOT 2 χ NC χ CDBM JTOT,JOH,JNB,JRF,JBS [MA/m 2 ] vs r j OH j BS j LH j TOT QP vs r q

19 Self-Consistent Wave Analysis with Modified f(u) Modification of velocity distribution from Maxwellian Absorption of ICRF waves in the presence of energetic ions Current drive efficiency of LHCD NTM controllability of ECCD (absorption width) Self-consistent wave analysis including modification of f (u)

20 Self-Consistent ICRF Minority Heating Analysis Analysis in TASK Dielectric tensor for arbitrary f (v) Full wave analysis with the dielectric tensor Fokker-Plank analysis of full wave results Self-consistent iterative analysis: Preliminary Energetic ion tail formation Broadening of power deposition profile Momentum Distribution Tail Formation Power deposition PPERP 10 0 F2 FMIN = E+01 FMAX = E P abs with tail Pabs [arb. unit] P abs w/o tail PPARA p**2 r/a

21 FLR Effects in Full Waves Analyses Several approaches to describe the FLR effects. Differential operators: k ρ iρ / r This approach cannot be applied to the case k ρ 1. Extension to the third and higher harmonics is difficult. Spectral method: Fourier transform in inhomogeneous direction This approach can be applied to the case k ρ>1. All the wave field spectra are coupled with each other. Solving a dense matrix equation requires large computer resources. Integral operators: ɛ(x x ) E(x )dx This approach can be applied to the case k ρ>1 Correlations are localized within several Larmor radii Necessary to solve a large band matrix

22 Full Wave Analysis Using an Integral Form of Dielectric Tensor Maxwell s equation: E(r) + ω2 ɛ (r, r c 2 ) E(r )dr = μ 0 j ext (r) Integral form of dielectric tensor: ɛ (r, r ) Integration along the unperturbed cyclotron orbit 1D analysis in tokamaks (in the direction of major radius) To confirm the applicability of an integral form of dielectric tensor Another formulation in the lowest order of ρ/l Sauter O, Vaclavik J, Nucl. Fusion 32 (1992) D analysis in tokamaks In more realistic configurations

23 One-Dimensional Analysis ICRF minoring heating with α-particles (n D : n He = 0.96 : 0.02) Differential form Integral form [V/m] [V/m] Ex Ey Ex Ey R 0 = 3.0m a = 1.2m B 0 = 3T T e0 = 10keV T D0 = 10keV [W/m 2] [W/m 2] PHe T α0 = 3.5MeV PD PHe Pe PD Pe n s0 = m 3 ω/2π = 45MHz Absorption by α may be overestimated by differential approach.

24 2-D Formulation Coordinates Magnetic coordinate system: (ψ, χ, ζ) Local Cartesian coordinate system: (s, p, h) Fourier expansion: poloidal and toroidal mode numbers, m, n Perturbed current j(r, t) = q du qu m dt [ E(r, t ) + u B(r, t ) ] f 0(u ) u The time evolution of χ and ζ due to gyro-motion χ(t τ) = χ(t) + χ v {cos(ω c τ + θ 0 ) cos θ 0 } + χ v {sin(ω c τ + θ 0 ) sin θ 0 } χ s ω c p ω c h v τ ζ(t τ) = ζ(t) + ζ v {cos(ω c τ + θ 0 ) cos θ 0 } + ζ s ω c p v {sin(ω c τ + θ 0 ) sin θ 0 } ζ ω c h v τ

25 Variable Transformations Transformation of Integral Variables Transformation from the velocity space variables (v,θ 0 ) to the particle position s and the guiding center position s 0. ω 2 c Jacobian: J = (v,θ 0 ) (s, s 0 ) = v sin ω c τ. Integration over τ Integral in time calculated by the Fourier series expansion with cyclotron period, 2π/ω c Integration over v Interaction between wave and particles along the magnetic field lines described by the plasma dispersion function.

26 Final Form of Induced Current Induced current: μ 1 1 (ψ) 2 (ψ) = 3 (ψ) J mn J mn J mn du du 0 σ (u, u, u 0 ) 1 (ψ) 2 (ψ) 3 (ψ) E m n E m n E m n Electrical conductivity: ( )7 1 2 σ (u, u q 2, u 0 ) = i n0 2π m Matrix coefficients: m n H 1i = ( ) Q 3 μ 1 1i u Q 1 μ 1 π 2i Z(η l ) + k v T l [ 2π H 2i = ( ) [ Q 2 uμ 1 1i + Q 0 uu μ 1 π 2i Z(η l ) + k v T H 3i = ( Q 2 μ 1 1i + Q 0u ) π μ 1 2i v T v T k Z (η l ) + dχ 2π 0 Q 1v T v 2 μ 1 3i + T dζ exp i { (m m)χ + (n n)ζ } H (u, u,χ) ( 1 v2 T v 2 T ( Q 0 uv T v 2 μ 1 3i T [ Q 0 μ 1 3i + v T v T v T 1 v2 T v 2 T ( ) {Q3 } ] π κ 2i + Q 1 u κ 1i 2 ) 1 v2 T v 2 T 1 k Z (η l ) u { Q 2 κ 2i + Q 0 u κ 1i } ] π 2 1 k Z (η l ) ) {Q2 κ 2i + Q 0 u κ 1i } ] π k η l Z (η l )

27 Kernel functions Q V 2 0 = (u, u,χ 0, l) = ( u + u 2 V 1 = u u 2 V 2 = u u 2 2π 0 exp i ) 2 1 cos λ + 1 tan 1 2 λ u + u 2 1 tan 1 2 λ + u + u 2 Kernel Functions dλ 1 sin λ 1 V 1 V 2 V 1 V 2 [ k v T { (V2 V 1 )cosα (u u )sinα } + lλ V2 0 ω c 2 ( ) u u tan 1 2 λ tan 1 2 λ sin λ h = 1 Jω u s s 0 ω c v T u s s 0 ω c v T 0 n m n 0 i ψ m i ψ 0 where κ = μ 1 g h, μ is the transformation matrix for (s, p, h) (ψ, χ, ζ), and g is the metric tensor. ]

28 Consistent Formulation of Integral Full Wave Analysis Analysis of wave propagation Dielectric tensor: E(r) ω2 c 2 dr 0 dr p f 0 (p, r 0 ) mγ p where r 0 is the gyrocenter position. K 1 (r, r, r 0 ) E(r ) = i ωμ 0 j ext Analysis of modification of momentum distribution function Quasi-linear operator f 0 t + ( ) f0 p E + p dr dr E(r) E(r ) K 2 (r, r, r 0 ) f 0(p, r 0, t) p = ( ) f0 The kernels K 1 and K 2 are closely related and localized in the region r r 0 ρ and r r 0 ρ. p col

29 Extension to TASK/3D 3D Equilibrium: Interface to equilibrium data from VMEC or HINT Interface to neoclassical transport coefficient codes Modules 3D-ready: WR: Ray and beam tracing WM: Full wave analysis Modules to be updated: TR: Diffusive transport (with an appropriate model of E r ) TX: Dynamic transport (with neoclassical toroidal viscosity) Modules to be added: (by Y. Nakamura) EI: Time evolution of current profile in helical geometry

30 Road map of TASK code Present Status In 2 years In 5 years Equlibrium Fixed/Free Boundary Equilibrium Evolution Start Up Analysis Core Transport 1D Diffusive TR Kinetic TR 2D Fluid TR 1D Dynamic TR SOL Transport 2D Fluid TR Plasma-Wall Interaction Neutral Tranport 1D Diffusive TR Orbit Following Energetic Ions Kinetic Evolution Orbit Following Wave Beam Ray/Beam Tracing Beam Propagation Full Wave Kinetic ε Gyro Integral ε Orbit Integral ε Stabilities Sawtooth Osc. Tearing Mode Systematic Stability Analysis ELM Model Resistive Wall Mode Turbulent Transport CDBM Model Linear GK + ZF Nonlinear ZK + ZF Diagnostic Module Control Module

31 Summary We are developing TASK code as a reference core code for integrated burning plasma simulation based on transport analysis. We have developed a part of standard dataset, data exchange interface and execution control and implemented them in TASK code. An example of coupling between TOPICS/EQU and TASK/TR was shown, though not yet completed. Some other modules of TOPICS will be incorporated soon. Preliminary results of self-consistent analysis of wave heating and current drive describing the time evolution of the momentum distribution function and Integro-differential full wave analysis including FLR effects have been obtained. Further continuous development of integrated modeling is needed for comprehensive ITER simulation.