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1D. McCune
PTRANSP
Predictive Upgrades for TRANSP
2D. McCune
US Predictive Modeling Effort
• R. Budny, S. Jardin, C. Kessel, L. P. Ku, D. McCune (PPPL).
• H. St. John (GA).
• D. P. Grote, L. Lodestro, L. D. Pearlstein, T. D. Rognlien (LLNL).
• G. Bateman, F. Halpern, A. Kritz (Lehigh).
• J. Carlsson (Tech-X).
3D. McCune
PTRANSP Plan• Leverage TRANSP:
– Well validated source models (NBI, alphas, ICRF, LH, ECH/ECCD).
– Strong connection to experimental data.– Fusion Grid production facility.
• Add predictive capabilities to TRANSP:– Robust transport equation solver.– Free boundary equilibrium.– Connection to edge model.
• Reuse existing software to extent possible.
4D. McCune
Design Principles - 1
• Reuse TRANSP and Fusion Simulation Project (FSP) software (to minimize costs).
• Two driver configurations:– Free boundary: (TRANSP computes sources;
analyzes free boundary code results).– Prescribed boundary: traditional TRANSP
with:• New transport solvers (FSP Solver, GCNM-P).• New MHD equilibrium solvers (FSP, TEQ).
5D. McCune
Design Principles - 2
• Modular design: interchangeability of critical parts (create/use NTCC modules):– Transport solvers.– MHD equilibrium solvers.– Sources.
• Leverage TRANSP archives:– Access to experimental data for validation.– NTCC module provided for data access.
6D. McCune
Solver Equilibrium Sources
GCNMP
FSP-Sol
Controller
TEQ
FSP-Equ
ESC
TRANSP
Plasma State
TRDATBUF (access to experimental data)
FSP-Src
XPLASMA (FSP upgrade in progress)
Edge AnalysisStability Analysis
Postprocessing (initially)
Sawtooth
Edge Pedestal
Bootstrap Curr
NCLASS
Hirsh-Sig.
Lehigh
PPPL
Porcelli-L
Porcelli-P
UEDGE
DEGAS-2
DCON
PEST-2
PTRANSP Schematic
TRANSP-based controller
FSP-based controller
7D. McCune
Transport Solver Dilemma
• Current predictive transport models (e.g. GLF-23) are very stiff.
• Standard numerical integration methods suffer severe oscillations and instability.
• Attempts to “smooth” GLF-23 directly significantly changes prediction results.
• Therefore: serious solver upgrade effort.– GCNM-P (General Atomics) & FSP (PPPL).
8D. McCune
Transport Solvers
• GCNM – Globally Convergent Newton Method – ONETWO Solver (St. John, GA).– Very general stiff PDE integrator.– Use of Jacobian, O(n**2) execution cost.
• FSP Solver (Jardin & Ku, PPPL).– “Local” Newton method– forward implicit use
of dependence of transport on grad(Ti,Te,…).– O(n) but may not be as stable as GCNM.
9D. McCune
The PTRANSP FSP Solver - 1This has been implemented in the full solver in the FSP:
Without linearization With linearization
• ITER simulation• Linearization of dependence of GLF-23 fluxes on temperature gradients.• Behavior reproducible in simplified single-T analytic transport model.• Caveat: DIII-D experimental data validation attempt– not yet fully stable.
S. Jardin / L. P. Ku
10D. McCune
The PTRANSP FSP Solver - 2Convergence Tests:
3 Newton iterations per timestep
Double # of zones Reduce timestep by 3
Base case: 1 Newton iteration per timestep
S. Jardin / L. P. Ku
11D. McCune
Results for a 500s ITER run:
Profiles at 250s
Chi Values for entire run
Powers vs time
ions
electrons
Chi vs radius at 250s
ions
electrons
S. Jardin / L. P. Ku
12D. McCune
PTRANSP Progress - 1
• Predictive Solver Improvement (as shown).– Both FSP solver and GCNM at GA.
• TRANSP Improvements:– Export of source calculation results.– Accommodation of free boundary equilibrium.– Modification of internal loop structure to allow
import of stiff transport solver results.
• Trdatbuf_lib NTCC module– access to TRANSP input data (experimental data).
13D. McCune
PTRANSP Progress - 2
• LLNL’s TEQ free boundary solver module in TRANSP.– NTCC module standards with error handling
enhancement.– Time dependent NSTX test results look good.
• UEDGE/TRANSP coupling:– LLNL design and prototype in place.– Includes TRANSP/UEDGE data exchange
schema.
14D. McCune
PTRANSP Progress - 3
• NTCC PEDESTAL module– predictive boundary condition option.– Lehigh University team making direct
modifications to TRANSP (in progress).– Prototype installation in BALDUR.– Experience with L to H transition dynamics.
15D. McCune
PTRANSP’s Next Step – APSPTRANSP’s Next Step – APS
• Drive TRANSP with ITER free boundary simulation:– TRANSP provides heating and current drive.– TRANSP uses free boundary simulation
predicted temperatures and equilibria.• Architecture compatible with density prediction but
testing of this capability likely to be postponed.
– TRANSP archive produced:• Available as input to UEDGE, linear stability
solvers, etc.
16D. McCune
Summary
• The PTRANSP project will provide a community predictive transport code with state-of-the-art capabilities.
• Like TRANSP itself, it will run as a Fusion Grid production service with world wide access.
• Control options will be provided for prescribed boundary or free boundary operation.
• Example of integrated ITER simulation with realistic sources by APS-2006.