FPT Discussions on Current Research Topics Z. Lin University of California, Irvine, California 92697, USA.

Slides:



Advertisements
Similar presentations
Magnetic Turbulence in MRX (for discussions on a possible cross-cutting theme to relate turbulence, reconnection, and particle heating) PFC Planning Meeting.
Advertisements

Magnetic Chaos and Transport Paul Terry and Leonid Malyshkin, group leaders with active participation from MST group, Chicago group, MRX, Wisconsin astrophysics.
Key Questions and Issues in turbulent Transport in Tokamaks JAEA M. Kikuchi 2 nd APTWG at Chengdu, Plenary session, presentation number PL-1 1PL-1 Acknowledgements:
Short wavelength ion temperature gradient driven instability in toroidal plasmas Zhe Gao, a) H. Sanuki, b) K. Itoh b) and J. Q. Dong c) a) Department of.
Lecture Series in Energetic Particle Physics of Fusion Plasmas Guoyong Fu Princeton Plasma Physics Laboratory Princeton University Princeton, NJ 08543,
A Kinetic-Fluid Model for Studying Thermal and Fast Particle Kinetic Effects on MHD Instabilities C. Z. Cheng, N. Gorelenkov and E. Belova Princeton Plasma.
6 th ITPA MHD Topical Group Meeting combined with W60 IEA Workshop on Burning Plasmas Session II MHD Stability and Fast Particle Confinement General scope.
Non-Resonant Quasilinear Theory Non-Resonant Theory.
Kinetic Theories of Geodesic Acoustic Modes in Toroidal Plasmas Zhiyong Qiu, F. Zonca and L. Chen IFTS, May 2010.
INTRODUCTION OF WAVE-PARTICLE RESONANCE IN TOKAMAKS J.Q. Dong Southwestern Institute of Physics Chengdu, China International School on Plasma Turbulence.
Alfvén-cyclotron wave mode structure: linear and nonlinear behavior J. A. Araneda 1, H. Astudillo 1, and E. Marsch 2 1 Departamento de Física, Universidad.
Modeling Generation and Nonlinear Evolution of Plasma Turbulence for Radiation Belt Remediation Center for Space Science & Engineering Research Virginia.
1 Global Gyrokinetic Simulations of Toroidal ETG Mode in Reversed Shear Tokamaks Y. Idomura, S. Tokuda, and Y. Kishimoto Y. Idomura 1), S. Tokuda 1), and.
Fast ion effects on fishbones and n=1 kinks in JET simulated by a non-perturbative NOVA-KN code TH/5-2Rb N.N. Gorelenkov 1), C.Z.Cheng 1), V.G. Kiptily.
Some results / ideas on the effect of flows D. Strintzi, C. Angioni, A. Bottino, A.G. Peeters.
GTC Status: Physics Capabilities & Recent Applications Y. Xiao for GTC team UC Irvine.
Large-scale structures in gyrofluid ETG/ITG turbulence and ion/electron transport 20 th IAEA Fusion Energy Conference, Vilamoura, Portugal, November.
Intermittent Transport and Relaxation Oscillations of Nonlinear Reduced Models for Fusion Plasmas S. Hamaguchi, 1 K. Takeda, 2 A. Bierwage, 2 S. Tsurimaki,
1 / 12 Association EURATOM-CEA IAEA 20th Fusion Energy Conference presented by Ph. Ghendrih S. Benkadda, P. Beyer M. Bécoulet, G. Falchetto,
Turbulent transport in collisionless plasmas: eddy mixing or wave-particle decorrelation? Z. Lin Y. Nishimura, I. Holod, W. L. Zhang, Y. Xiao, L. Chen.
Nonlinear Frequency Chirping of Alfven Eigenmode in Toroidal Plasmas Huasen Zhang 1,2 1 Fusion Simulation Center, Peking University, Beijing , China.
Wave-Particle Interaction in Collisionless Plasmas: Resonance and Trapping Zhihong Lin Department of Physics & Astronomy University of California, Irvine.
Joaquim Loizu P. Ricci, F. Halpern, S. Jolliet, A. Mosetto
Gyrokinetic Simulation of Energetic Particle Turbulence and Transport Zhihong Lin University of California, Irvine & UCI: L. Chen, W. Heidbrink, A. Bierwage,
Kinetic Effects on the Linear and Nonlinear Stability Properties of Field- Reversed Configurations E. V. Belova PPPL 2003 APS DPP Meeting, October 2003.
Calculations of Gyrokinetic Microturbulence and Transport for NSTX and C-MOD H-modes Martha Redi Princeton Plasma Physics Laboratory Transport Task Force.
Particle-in-Cell Simulations of Electron Transport from Plasma Turbulence: Recent Progress in Gyrokinetic Particle Simulations of Turbulent Plasmas Z.
TH/7-2 Radial Localization of Alfven Eigenmodes and Zonal Field Generation Z. Lin University of California, Irvine Fusion Simulation Center, Peking University.
Interplay between energetic-particle-driven GAMs and turbulence D. Zarzoso 15 th European Fusion Theory Conference, Oxford, September CEA, IRFM,
Challenging problems in kinetic simulation of turbulence and transport in tokamaks Yang Chen Center for Integrated Plasma Studies University of Colorado.
Excitation of ion temperature gradient and trapped electron modes in HL-2A tokamak The 3 th Annual Workshop on Fusion Simulation and Theory, Hefei, March.
Presented by Gyrokinetic Particle Simulations of Fusion Plasmas Scott A. Klasky Scientific Computing National Center for Computational Sciences.
Recent advances in wave kinetics
Summary of MHD Topics 2nd IAEA Technical Meeting Theory of Plasma Instabilities Howard Wilson.
Lecture Series in Energetic Particle Physics of Fusion Plasmas
CCFE is the fusion research arm of the United Kingdom Atomic Energy Authority Internal Transport Barriers and Improved Confinement in Tokamaks (Three possible.
11 Role of Non-resonant Modes in Zonal Flows and Intrinsic Rotation Generation Role of Non-resonant Modes in Zonal Flows and Intrinsic Rotation Generation.
Stability Properties of Field-Reversed Configurations (FRC) E. V. Belova PPPL 2003 International Sherwood Fusion Theory Conference Corpus Christi, TX,
Dynamics of ITG driven turbulence in the presence of a large spatial scale vortex flow Zheng-Xiong Wang, 1 J. Q. Li, 1 J. Q. Dong, 2 and Y. Kishimoto 1.
Gyrokinetic Particle Simulation of Plasma Turbulence Zhihong Lin Department of Physics & Astronomy University of California, Irvine Workshop on ITER Simulation.
Nonlinear interactions between micro-turbulence and macro-scale MHD A. Ishizawa, N. Nakajima, M. Okamoto, J. Ramos* National Institute for Fusion Science.
Comparison of Ion Thermal Transport From GLF23 and Weiland Models Under ITER Conditions A. H. Kritz 1 Christopher M. Wolfe 1 F. Halpern 1, G. Bateman 1,
Association EURATOM-CEA Electromagnetic Self-Organization and Turbulent Transport in Tokamaks G. Fuhr, S. Benkadda, P. Beyer France Japan Magnetic Fusion.
Lecture Series in Energetic Particle Physics of Fusion Plasmas Guoyong Fu Princeton Plasma Physics Laboratory Princeton University Princeton, NJ 08543,
A discussion of tokamak transport through numerical visualization C.S. Chang.
Effects of Flow on Radial Electric Fields Shaojie Wang Department of Physics, Fudan University Institute of Plasma Physics, Chinese Academy of Sciences.
Alfven Waves in Toroidal Plasmas
Summary of IAEA Theory Papers on Energetic Particle Physics Guoyong Fu.
Summary on transport IAEA Technical Meeting, Trieste Italy Presented by A.G. Peeters.
Princeton Plasma Physics Laboratory Highlights of Theory Accomplishments and Plans Department of Energy Budget Planning Meeting March 13-15, 2001.
SMK – APS ‘06 1 NSTX Addresses Transport & Turbulence Issues Critical to Both Basic Toroidal Confinement and Future Devices NSTX offers a novel view into.
Y. Kishimoto 1,2), K. Miki 1), N. Miyato 2), J.Q.Li 1), J. Anderson 1) 21 st IAEA Fusion Energy Conference IAEA-CN-149-PD2 (Post deadline paper) October.
Simulations of turbulent plasma heating by powerful electron beams Timofeev I.V., Terekhov A.V.
TTF M. Ottaviani Euratom TORE SUPRA Overview of progress in transport theory and in the understanding of the scaling laws M. Ottaviani EURATOM-CEA,
Helically Symmetry Configuration Evidence for Alfvénic Fluctuations in Quasi-Helically Symmetric HSX Plasmas C. Deng and D.L. Brower, University of California,
Simulations of Energetic Particle Modes In Spherical Torus G.Y. Fu, J. Breslau, J. Chen, E. Fredrickson, S. Jardin, W. Park Princeton Plasma Physics Laboratory.
Nonlinear Simulations of Energetic Particle-driven Modes in Tokamaks Guoyong Fu Princeton Plasma Physics Laboratory Princeton, NJ, USA In collaboration.
Kinetic-Fluid Model for Modeling Fast Ion Driven Instabilities C. Z. Cheng, N. Gorelenkov and E. Belova Princeton Plasma Physics Laboratory Princeton University.
IAEA-TM 02/03/2005 1G. Falchetto DRFC, CEA-Cadarache Association EURATOM-CEA NON-LINEAR FLUID SIMULATIONS of THE EFFECT of ROTATION on ION HEAT TURBULENT.
Interaction between vortex flow and microturbulence Zheng-Xiong Wang (王正汹) Dalian University of Technology, Dalian, China West Lake International Symposium.
Transport Model with Global Flow M. Yagi, M. Azumi 1, S.-I. Itoh, K. Itoh 2 and A. Fukuyama 3 Research Institute for Applied Mechanics, Kyushu University.
TH/7-1Multi-phase Simulation of Alfvén Eigenmodes and Fast Ion Distribution Flattening in DIII-D Experiment Y. Todo (NIFS, SOKENDAI) M. A. Van Zeeland.
An overview of turbulent transport in tokamaks
IAEA Fusion Energy Conference 2012, 8-13 Oct., San Diego, USA
Gyrokinetic Simulation of Multimode Plasma Turbulence
Huishan Cai, Jintao Cao, Ding Li
Influence of energetic ions on neoclassical tearing modes
Stabilization of m/n=1/1 fishbone by ECRH
Instability and Transport driven by ITG mode
Ioffe Summary Fast MHD oscillations observed on the TUMAN-3M in absence of energetic ions Bursts of the oscillations correlate with saw-tooth crashes and.
Presentation transcript:

FPT Discussions on Current Research Topics Z. Lin University of California, Irvine, California 92697, USA

Electron transport Momentum transport GAM Finite-  effects Coupling between turbulence and energetic particles Outline

Case studies of electron heat transport mechanism in tokamak  Comparative studies of CTEM, ITG, & ETG GTC simulations: while saturation can be understood in context of fluid processes, kinetic processes related to instability drive often responsible for transport Transport: eddy mixing or wave-particle decorrelation? InstabilityElectron temperature gradient (ETG) Ion temperature gradient (ITG) Collisionless trapped electron mode (CTEM) Electron driveParallel resonanceNon-resonancePrecessional resonance SaturationNonlinear toroidal coupling Zonal flows Electron heat Transport Wave-particle decorrelation Nonlinear mode scattering off trapped electron? Processional resonance de-tuning? Avalanche?

Transport driven by local fluctuation intensity Effective wave-particle decorrelation time  wp =4  e /3  v r 2 ~ 4.2L T / v e  wp << 1/  ~ 33: linear time scale not important to transport Wave-particle correlation length  v r  wp << streamer length Electron radial excursion diffusive: streamer length does not determine transport directly From linear to nonlinear,  e /  v r 2 decreases by a factor of ~5  Nonlinear loss of wave-particle correlation r/er/e ee e/vr2e/vr2 time (L T /v e )

Kinetic & fluid time scales in ETG turbulence  auto >> 1/  >>  wp ~ 1/  k || v e Wave-particle decorrelation of parallel resonance  (  -k || v || ) dominates Quasilinear calculation of  e agrees well with simulation Saturation: wave-wave coupling determines fluctuation intensity Transport: wave-particle decorrelation determines transport level

ITG mode dominates when  i =3.1 Trapped electrons typically interact non-resonantly with ITG mode Trapped electrons increase ITG growth rate High k  modes are CTEM Effects of kinetic electrons on ITG mode k   i  ( v i / L n )  r ( v i / L n ) k   i kinetic electron kinetic electron adiabatic electron adiabatic electron

Convergence using 10 and 40 particles per cell No coherent ITG-electron interaction in linear phase Ion transport: resonant; proportional to intensity [ Lin & Hahm, PoP2004 ] Electron transport: non-resonant  ITG mode scattering off trapped electrons? Relation to energetic particle transport by microturbulence? ITG turbulence drive small electron heat transport heat flux electron ion   ion electron

CTEM mode dominates when  i =1 Driven by electron precessional resonance Modestly ballooning CTEM linear dispersion

Nonlinear convergence using particle per cell Short wavelength modes k   i >0.4 dominate at initial saturation Initial saturation caused by small scale zonal flows k r  i ~1 The 2 nd burst not deterministic; driven by k   i <0.4 Nonlinear saturation time (1/  )

Nonlinear loss of CTEM-electron correlation  Zonal flow the agent? Burst caused by nonlinear growth Electron heat transport mechanism: precessional resonance de-tuning?  n-spectral width; Radial diffusion Nonlinear burst suggestive of avalanche? Nonlinear bursting

Burst originates at r=0.5a, outward propagation faster than inward Inward spreading ballistic with a speed close to drift velocity Relation to EPM avalanche [Zonca, Briguglio, Vlad, etal, PPCF2006]? Nonlinear bursting time (1/  ) ii ee r/  i Ion transport Electron transport

Nonlocality in TransportSecondary modes and structures Strong wave-particle interaction Particle Transport enhanced particle transport by avalanches and spreading shearing and zonal flow effects and particle pinch CTEM induced particle transport EPM induced transport Electron Thermal Transport resonant electron, CTEM induced avalanches Zonal flow and GAM effects on CTEM CTEM induced heat transport electron heat avalanches precession resonance coherence ITB Formation avalanche-barrier interaction spreading vs. barrier competition. Interplay of GAM and shear flows Intrinsic rotation in ITB shear layers CTEM resonance detuning in electron ITB shearing effects on CTEM Transport scalings Gyro-Bohm breaking  spreading and avalanches probabilistic heat flux scaling interplay collisionless GAM, ZF saturation  stiffness quantification CTEM dynamics precession resonance coherence  radial front propagation Momentum Transport wave momentum flux and spreading enhancement driven intrinsic rotation. symmetry breaking energetic ions  Alfven wave momentum flux CTEM, KBM driven momentum flux

GAM linear physics: short wavelength, collisionless & collisional damping Nonlinear excitation: turbulence & zonal flows Effects on turbulence: active or passive? Role of quasimodes? Acoustic eigenmode? Higher frequency harmonics? EM: roles of low-order rational surfaces in driving ZF & GAM? Geodesic Acoustic Modes & Zonal Flow

GTC electromagnetic simulation   e (v e  e 2 /L T ) time (L T /v e ) Demonstrate finite-  stabilization of ITG and excitation of KBM/AITG Demonstrate Alfven wave propagation in tokamak, continuum damping, and existence of toroidal frequency gap  Truly global geometry allowing all n -modes  Recover MHD dispersion relation of Alfven wave in tokamak; Allow E || [ Nishimura, Lin, and Wang, PoP2007 ]

Coupling of TT & EP in ITER: turbulence in the presence of energetic particles; Many interacting EP modes lead to EP turbulence Kinetic effects of thermal ions: damping of TAE; coupling between Alfvenic and acoustic branches, e.g., GBAAE Cross-gap coupling between Alfvenic and acoustic modes Cross-scale coupling between TT & EP, e.g., coherent structures (zonal flows/fields), structure corrugation & dynamic modulation Turbulent transport & energetic particle physics

Fundamental constituents Fundamental constituents Derived Observables Primacy hierarchy Linear SAW wave Nonlinear saturation TransportScaling Trend Statistics ObservablesPolarization, structure, frequency, threshold Spectral intensity, bispectra, zonal flows/fields EP PDF & transport Similarity experiment ITPA database Agent/ mechanism EP spatial gradient, velocity anisotropy Wave-wave, wave-particle interaction Cross- phase, relaxation Dimensionle ss scaling Inter- machine