Bounce-averaged gyrokinetic simulations of trapped electron turbulence in elongated tokamak plasmas
|
|
- Dina Parrish
- 5 years ago
- Views:
Transcription
1 Bounce-averaged gyrokinetic simulations of trapped electron turbulence in elongated tokamak plasmas Lei Qi a, Jaemin Kwon a, T. S. Hahm a,b and Sumin Yi a a National Fusion Research Institute (NFRI), Daejeon, Korea b Seoul National University (SNU), Seoul, Korea address: qileister@nfri.re.kr 1
2 2 Outlines I. Motivation II. Nonlinear verification of bounce-averaged gyrokinetic simulation III. Elongation effects on CTEM driven turbulence and transport Transport Zonal flow Turbulence IV. Conclusions and future work
3 3 I. Motivation ITG Adiabatic electrons low computational cost (large time step, simple Poisson eqn., etc.) TEM kinetic trapped electrons large computational cost (small time step, complicate Poisson eqn., etc.) TEM Bounce-averaged kinetic trapped electron reduce computation cost (time step issue is resolved) Previous trial of bounce-averaged gyrokinetic simulation scheme is limited on linear simulations [Y. Idomura et al., J. Plasma Fusion, Res. (2004); G. Rewoldt et al., CPC (2007)]. No nonlinear reports. Recently, both linear [L. Qi, J.-M. Kwon, T. S. Hahm et al., PoP (2016)] and nonlinear [J.-M. Kwon, L. Qi, T. S. Hahm et al., CPC (2017)] bounced-averaged gyrokinetic simulations are achieved. efficient ITG-TEM simulations Empirical ITER IPB98(y,2) H-mode confinement scaling τ E κ 0.78 (κ is elongation) This motivated previous GK simulation on ITG [Angelino et al., PRL (2009); Villard et al., PPCF (2013)]. No work yet is devoted to investigating elongation effects on TEM.
4 II-1 Toward Nonlinear Simulation In nonlinear state, particles are scattered by fluctuation in phase space i.e. trap passing Coulomb collision is another important mechanism in the mixing We need to model passing electrons and their mixing with trapped population subcycling drift kinetic electrons, which are passively following the evolution of fluctuation v Trapped particles v 2 v 2 = 1 B B max Passing particles Passing particles v 4
5 5 II-2 Coulomb Collision Electron pitch angle (λ = v /v) scattering by Lorentz collision 1 C L f e = ν e 2 λ 1 λ2 λ f e passing and trapped particle distributions are smoothly connected Analytic Maxwellian distribution Numerical electron distribution with collision
6 6 II-3 Nonlinear verification Particle number convergence test (a) Electron heat diffusivity (b) Zonal flow shearing rate
7 7 II-3 Nonlinear verification (Cont.) Linear TEM growth rates [J.-M. Kwon, L. Qi, T. S. Hahm et al., CPC (2017)] Nonlinear results: (a) electron heat diffusivity; (b) zonal flow shearing rate
8 8 II-4 Efficiency Overall distribution of computational costs 200 ~ 300% increase of simulation time compared to adiabatic ITG case Component Computational Cost Ions 17% Trapped electrons 27% Passing electrons 17% Deposition and Poisson solver 34% Collision 5%
9 9 II-5 Code summary Code: GyroKinetic Plasma Simulation Program (gkpsp), linear and nonlinear version δf, Global gyrokinetic code (GK ions) Bounce-averaged kinetic trapped electrons Particle-In-Cell (PIC) code Zonal flow conserving Krook operator to control noise Heating source to control density and temperature profiles 3D tokamak geometry including circular, analytical shaping, and experimental shaping equilibria
10 III-1 Setup We select a Collisionless Trapped Electron Mode (CTEM). Main parameters are the following at reference plane r = 0.5a: (initial setup) R 0 = 1.86m, a = 0.666m, B 0 = 1.91T, T e = 2.5keV, n e = m 3, m i m e = 1836 R 0 L Te = 6.9, R 0 L Ti = 2.2 R 0 L n = 2.2 a ρ i = 250 T i T e = 1 q = r a (r/a) 2 s = Gradients locate at [0.25a, 0.75a]
11 11 III-2 Setup (Cont.) Linear gkpsp simulations show that for elongations κ = 1.0 and 2.0 growth rates of this CTEM case are nearly the same in terms of effective poloidal wave numbers. To separate linear and nonlinear effects. In the viewpoint of linear growth rates, the same linear drive, differences in the nonlinear saturation mechanism could be investigated. Nonlinear setup: Particle markers: N i = 200 per mode, N trapped electron = 40 per mode Simulation domain: r 0.1a, 1.0a, dr~ρ i Run with κ = 1.0, maximum toroidal mode number n max = 124, 1/4 of torus 32 modes Run with κ = 2.0, maximum toroidal mode number n max = 248, 1/8 of torus 32 modes (maximum effective poloidal wave number k θ ρ i /κ~1.4)
12 III-3 Linear background ITG-TEM mode actually feels the effective poloidal wave number k θ ρ i /κ. 12 Frequency of ITG-TEM mode as a function of the poloidal wave number k θ ρ i (Left figure) and the effective poloidal wave number k θ ρ i /κ (Right figure) for elongations of κ = 1.0, 1.25 and 1.5. Ref: Lei Qi, J.M. Kwon et al, PoP2016 k θ eff θ = 0 = nq r 1 κ ε2 nq r 1 κ = k θ κ.
13 13 III-4 Transport Elongation effects on transport: Nonlinear stabilizations Transport burst is observed, and persist independently of Elongation introduces more evident radial fine structures in χ i. Ion heat transport more localized than electron heat transport, elongation enhances the localization. D < χ i < χ e for both elongations Γ = D n Q i = n 0 χ i T i Q e = n tr χ e T e
14 14 III-5 Zonal flow (1) Zonal flow shearing Reduce turbulence transport Elongation enhances zonal flow shearing rate 1. In radially average (Fig. c) 2. Especially at outer of midradius (2) Radial fine structures Larger radial wave numbers k r 0.5, 1.0 (by TEM) [Y. Xiao et al., PoP (2010)] Elongation shows a stronger spectrum that locates at relatively larger radial wave number
15 15 III-6 Radial scales Scale of turbulence eddies another factor to affect transport radial correlation Two point correlation function C rζ Δr, Δζ = <δφ r+ r,ζ+δζ δφ r,ζ > <δφ 2 r+ r,ζ+δζ ><δφ 2 r,ζ >, at θ = 0 By taking maxima along the ridge of C rζ Δr, Δζ, we obtain C r Δr Two length scales in both elongations: Microscopic: L r ~4ρ i κ = 1.0 L r ~3ρ i κ = 2.0 Mesoscopic : larger L r Consistent with previous simulations [Y. Xiao et al., PRL (2009)] and experimental results [P. Hennequin et al., 42 nd EPS Conf. (2015)] Elongation reduces radial correlation in both microscopic and mesoscopic scales.
16 16 III-7 Turbulence spectrum For κ = 2: (around r=0.635a) A dual mode propagating in counter directions (ion diamagnetic and electron diamagnetic directions) With the occurrence of dual mode, stronger shearing rate is observed along with lower transport level. Similar observation has been made from experiments in the edge across L-H transition on DIII-D[Z. Yan, Submitted to NF (2017)]
17 17
18 18
19 19
20 20
21 IV Conclusions Nonlinear bounce-averaged gyrokinetic simulation is now ready for efficient ITG- TEM investigations. Further topics can be nonlinear ITG-TEM coupling and collisional effects, etc.. Nonlinear effects of plasma elongation on turbulence, zonal flow and transport in isolation from linear physics, are explicitly explored by efficient bounceaveraged global gyrokinetic simulations for CTEM. 21 Plasma elongation can stabilize both electron and ion heat fluxes as well as particle flux in CTEM dominant turbulence transport. Higher elongation is found to enhance the shorter radial scale zonal flows, and thus to lower transport levels. Two radial characteristic scales of turbulence eddies, i.e., microscopic and mesoscopic scales are observed in semi-quantitative agreements with previous simulations [Y. Xiao et al., PRL (2009)] and experimental results [P. Hennequin et a., 42 nd EPS Conf. (2015)]. Plasma elongation reduces both radial scales. A dual mode propagating in counter directions is observed with stronger sheared zonal flow for higher elongation.
22 22
23 23 III-7 Turbulence potential Turbulence potential amplitude e δφ /T, could affect transport level as well Elongation reduces turbulence amplitude
24 24 III-9 Global κ-scaling and role of zonal flow Global κ-scaling from gkpsp shows χ i κ 1.4, χ e κ 0.9, D κ 1.4 Due to κ itself, without shearing Empirical ITER IPB98(y,2) H-mode confinement scaling τ E κ 0.78 GYRO local simulations claimed scaling of κ 1, however mainly due to local κ shearing. It is evident that zonal flow plays significant roles in turbulence suppression with elongation
GTC Simulation of Turbulence and Transport in Tokamak Plasmas
GTC Simulation of Turbulence and Transport in Tokamak Plasmas Z. Lin University it of California, i Irvine, CA 92697, USA and GPS-TTBP Team Supported by SciDAC GPS-TTBP, GSEP & CPES Motivation First-principles
More informationSize Scaling and Nondiffusive Features of Electron Heat Transport in Multi-Scale Turbulence
Size Scaling and Nondiffusive Features of Electron Heat Transport in Multi-Scale Turbulence Z. Lin 1, Y. Xiao 1, W. J. Deng 1, I. Holod 1, C. Kamath, S. Klasky 3, Z. X. Wang 1, and H. S. Zhang 4,1 1 University
More informationProgress and Plans on Physics and Validation
Progress and Plans on Physics and Validation T.S. Hahm Princeton Plasma Physics Laboratory Princeton, New Jersey Momentum Transport Studies: Turbulence and Neoclassical Physics Role of Trapped Electrons
More informationGyrokinetic Transport Driven by Energetic Particle Modes
Gyrokinetic Transport Driven by Energetic Particle Modes by Eric Bass (General Atomics) Collaborators: Ron Waltz, Ming Chu GSEP Workshop General Atomics August 10, 2009 Outline I. Background Alfvén (TAE/EPM)
More informationTURBULENT TRANSPORT THEORY
ASDEX Upgrade Max-Planck-Institut für Plasmaphysik TURBULENT TRANSPORT THEORY C. Angioni GYRO, J. Candy and R.E. Waltz, GA The problem of Transport Transport is the physics subject which studies the physical
More informationZ. Lin University of California, Irvine, CA 92697, USA. Supported by SciDAC GPS-TTBP, GSEP & CPES
GTC Framework Development and Application Z. Lin University of California, Irvine, CA 92697, USA and dgpsttbp GPS-TTBP Team Supported by SciDAC GPS-TTBP, GSEP & CPES GPS-TTBP Workshop on GTC Framework
More informationParticle-in-cell simulations of electron transport from plasma turbulence: recent progress in gyrokinetic particle simulations of turbulent plasmas
Institute of Physics Publishing Journal of Physics: Conference Series 16 (25 16 24 doi:1.188/1742-6596/16/1/2 SciDAC 25 Particle-in-cell simulations of electron transport from plasma turbulence: recent
More informationValidation Study of gyrokinetic simulation (GYRO) near the edge in Alcator C-Mod ohmic discharges
Validation Study of gyrokinetic simulation (GYRO) near the edge in Alcator C-Mod ohmic discharges C. Sung, A. E. White, N. T. Howard, D. Mikkelsen, C. Holland, J. Rice, M. Reinke, C. Gao, P. Ennever, M.
More informationGlobal Nonlinear Simulations of Ion and Electron Turbulence Usintg a Particle-In-Cell Approach
Global Nonlinear Simulations of Ion and Electron Turbulence Usintg a Particle-In-Cell Approach S. Jolliet 1), B. F. McMillan 1), T. M. Tran 1), X. Lapillonne 1), L. Villard 1), A. Bottino 2), P. Angelino
More informationEntropy evolution and dissipation in collisionless particle-in-cell gyrokinetic simulations
Max-Planck-Insititut für Plasmaphysik Entropy evolution and dissipation in collisionless particle-in-cell gyrokinetic simulations A. Bottino Objectives Develop a numerical tool able to reproduce and predict
More informationUCIrvine. Gyrokinetic Studies of Turbulence Spreading IAEA-CN-116/TH1-4
AEA-CN-116/TH1-4 Gyrokinetic Studies of Turbulence Spreading T.S. Hahm, Z. Lin, a P.H. Diamond, b G. Rewoldt, W.X. Wang, S. Ethier, O. Gurcan, b W. Lee, and W.M. Tang Princeton University, Plasma Physics
More informationTurbulence and transport reduction with innovative plasma shapes in TCV - correlation ECE measurements and gyrokinetic simulations
Turbulence and transport reduction with innovative plasma shapes in TCV - correlation ECE measurements and gyrokinetic simulations A. Pochelon, and the TCV team 1 Ecole Polytechnique de Lausanne (EPFL)
More informationInternational Workshop on the Frontiers of Modern Plasma Physics July On the Nature of Plasma Core Turbulence.
1953-43 International Workshop on the Frontiers of Modern Plasma Physics 14-25 July 2008 On the Nature of Plasma Core Turbulence. F. Jenko Max-Planck Institute fuer Plasmaphysik Garching bei Munchen Germany
More informationAdvances in stellarator gyrokinetics
Advances in stellarator gyrokinetics Per Helander and T. Bird, F. Jenko, R. Kleiber, G.G. Plunk, J.H.E. Proll, J. Riemann, P. Xanthopoulos 1 Background Wendelstein 7-X will start experiments in 2015 optimised
More informationInvestigation of Intrinsic Rotation Dependencies in Alcator C-Mod
Investigation of Intrinsic Rotation Dependencies in Alcator C-Mod D. Kwak, A. E. White, J. E. Rice, N. T. Howard, C. Gao, M. L. Reinke, M. Greenwald, C. Angioni, R. M. McDermott, and the C-Mod and ASDEX
More informationFine-Scale Zonal Flow Suppression of Electron Temperature Gradient Turbulence
Fine-Scale Zonal Flow Suppression of Electron Temperature Gradient Turbulence S.E. Parker, J.J. Kohut, Y. Chen, Z. Lin, F.L. Hinton and W.W. Lee Center for Integrated Plasma Studies, University of Colorado,
More informationProperties of freely decaying and driven turbulence of fusion plasmas using gyrokinetic particle simulation
J. Plasma Fusion Res. SERIES, Vol. 9 () Properties of freely decaying and driven turbulence of fusion plasmas using gyrokinetic particle simulation R. Ganesh Institute for Plasma Research, Bhat Village,
More informationNeoclassical transport
Neoclassical transport Dr Ben Dudson Department of Physics, University of York Heslington, York YO10 5DD, UK 28 th January 2013 Dr Ben Dudson Magnetic Confinement Fusion (1 of 19) Last time Toroidal devices
More informationMulti-scale turbulence, electron transport, and Zonal Flows in DIII-D
Multi-scale turbulence, electron transport, and Zonal Flows in DIII-D L. Schmitz1 with C. Holland2, T.L. Rhodes1, G. Wang1, J.C. Hillesheim1, A.E. White3, W. A. Peebles1, J. DeBoo4, G.R. McKee5, J. DeGrassie4,
More informationGyrokinetic Turbulence in Tokamaks and Stellarators
Gyrokinetic Turbulence in Tokamaks and Stellarators Frank Jenko IPP, Germany Acknowledgements: P. Xanthopoulos, F. Merz, T. Görler, M. Pueschel, D. Told; A. Boozer, G. Hammett, D. Mikkelsen, M. Zarnstorff,
More informationTheory for Neoclassical Toroidal Plasma Viscosity in a Toroidally Symmetric Torus. K. C. Shaing
Theory for Neoclassical Toroidal Plasma Viscosity in a Toroidally Symmetric Torus K. C. Shaing Plasma and Space Science Center, and ISAPS, National Cheng Kung University, Tainan, Taiwan 70101, Republic
More informationCoarse-graining the electron distribution in turbulence simulations of tokamak plasmas
Coarse-graining the electron distribution in turbulence simulations of tokamak plasmas Yang Chen and Scott E. Parker University of Colorado at Boulder Gregory Rewoldt Princeton Plasma Physics Laboratory
More informationTransport Improvement Near Low Order Rational q Surfaces in DIII D
Transport Improvement Near Low Order Rational q Surfaces in DIII D M.E. Austin 1 With K.H. Burrell 2, R.E. Waltz 2, K.W. Gentle 1, E.J. Doyle 8, P. Gohil 2, C.M. Greenfield 2, R.J. Groebner 2, W.W. Heidbrink
More informationThe gyrokinetic turbulence code GENE - Numerics and applications
Contributors: T. Dannert (1), F. Jenko (1),F. Merz (1), D. Told (1), X. Lapillonne (2), S. Brunner (2), and others T. Görler (1) The gyrokinetic turbulence code GENE - Numerics and applications (1) Max-Planck-Institut
More informationTowards Multiscale Gyrokinetic Simulations of ITER-like Plasmas
Frank Jenko Max-Planck-Institut für Plasmaphysik, Garching Universität Ulm Towards Multiscale Gyrokinetic Simulations of ITER-like Plasmas 23 rd IAEA Fusion Energy Conference 11-16 October 2010, Daejeon,
More informationMicrotearing Simulations in the Madison Symmetric Torus
Microtearing Simulations in the Madison Symmetric Torus D. Carmody, P.W. Terry, M.J. Pueschel - University of Wisconsin - Madison dcarmody@wisc.edu APS DPP 22 Overview PPCD discharges in MST have lower
More informationGlobal gyrokinetic particle simulations with kinetic electrons
IOP PUBLISHING Plasma Phys. Control. Fusion 49 (2007) B163 B172 PLASMA PHYSICS AND CONTROLLED FUSION doi:10.1088/0741-3335/49/12b/s15 Global gyrokinetic particle simulations with kinetic electrons Z Lin,
More informationNSTX. Investigation of electron gyro-scale fluctuations in the National Spherical Torus Experiment. David Smith. Advisor: Ernesto Mazzucato
NSTX Supported by Investigation of electron gyro-scale fluctuations in the National Spherical Torus Experiment David Smith Advisor: Ernesto Mazzucato Final public oral exam February 26, 2009 Investigation
More informationValidation studies on local gyrokinetic simulations of tokamak ITG-TEM driven turbulent transport
Validation studies on local gyrokinetic simulations of tokamak ITG-TEM driven turbulent transport *Motoki Nakata 1, Mitsuru Honda 1, Maiko Yoshida 1, Hajime Urano 1, Shinya Maeyama 1, Masanori Nunami 2,
More informationUnderstanding and Predicting Profile Structure and Parametric Scaling of Intrinsic Rotation. Abstract
Understanding and Predicting Profile Structure and Parametric Scaling of Intrinsic Rotation W. X. Wang, B. A. Grierson, S. Ethier, J. Chen, and E. Startsev Plasma Physics Laboratory, Princeton University,
More informationGyrokinetic Simulations of Tokamak Microturbulence
Gyrokinetic Simulations of Tokamak Microturbulence W Dorland, Imperial College, London With key contributions from: S C Cowley F Jenko G W Hammett D Mikkelsen B N Rogers C Bourdelle W M Nevins D W Ross
More informationTheory Work in Support of C-Mod
Theory Work in Support of C-Mod 2/23/04 C-Mod PAC Presentation Peter J. Catto for the PSFC theory group MC & LH studies ITB investigations Neutrals & rotation BOUT improvements TORIC ICRF Mode Conversion
More informationTurbulence and Transport The Secrets of Magnetic Confinement
Turbulence and Transport The Secrets of Magnetic Confinement Presented by Martin Greenwald MIT Plasma Science & Fusion Center IAP January 2005 FUSION REACTIONS POWER THE STARS AND PRODUCE THE ELEMENTS
More informationC-Mod Transport Program
C-Mod Transport Program PAC 2006 Presented by Martin Greenwald MIT Plasma Science & Fusion Center 1/26/2006 Introduction Programmatic Focus Transport is a broad topic so where do we focus? Where C-Mod
More informationGyrokinetic simulations including the centrifugal force in a strongly rotating tokamak plasma
Gyrokinetic simulations including the centrifugal force in a strongly rotating tokamak plasma F.J. Casson, A.G. Peeters, Y. Camenen, W.A. Hornsby, A.P. Snodin, D. Strintzi, G.Szepesi CCFE Turbsim, July
More informationGlobal particle-in-cell simulations of Alfvénic modes
Global particle-in-cell simulations of Alfvénic modes A. Mishchenko, R. Hatzky and A. Könies Max-Planck-Institut für Plasmaphysik, EURATOM-Association, D-749 Greifswald, Germany Rechenzentrum der Max-Planck-Gesellschaft
More informationMagnetically Confined Fusion: Transport in the core and in the Scrape- off Layer Bogdan Hnat
Magnetically Confined Fusion: Transport in the core and in the Scrape- off Layer ogdan Hnat Joe Dewhurst, David Higgins, Steve Gallagher, James Robinson and Paula Copil Fusion Reaction H + 3 H 4 He + n
More informationLong Time Simulations of Microturbulence in Fusion Plasmas
Long Time Simulations of Microturbulence in Fusion Plasmas W. W. Lee, S. Ethier, T. G. Jenkins, W. X. Wang, J. L. V. Lewandowski, G. Rewoldt, and W. M. Tang Princeton Plasma Physics Laboratory, Princeton,
More informationGyrokinetics an efficient framework for studying turbulence and reconnection in magnetized plasmas
Frank Jenko Gyrokinetics an efficient framework for studying turbulence and reconnection in magnetized plasmas Max-Planck-Institut für Plasmaphysik, Garching Workshop on Vlasov-Maxwell Kinetics WPI, Vienna,
More informationMechanisms of intrinsic toroidal rotation tested against ASDEX Upgrade observations
Mechanisms of intrinsic toroidal rotation tested against ASDEX Upgrade observations William A. Hornsby C. Angioni, E. Fable, P. Manas, R. McDermott, Z.X. Lu, S. Grosshauser 2, A. G. Peeters 2 and the ASDEX
More informationA Simulation Model for Drift Resistive Ballooning Turbulence Examining the Influence of Self-consistent Zonal Flows *
A Simulation Model for Drift Resistive Ballooning Turbulence Examining the Influence of Self-consistent Zonal Flows * Bruce I. Cohen, Maxim V. Umansky, Ilon Joseph Lawrence Livermore National Laboratory
More informationDIAGNOSTICS FOR ADVANCED TOKAMAK RESEARCH
DIAGNOSTICS FOR ADVANCED TOKAMAK RESEARCH by K.H. Burrell Presented at High Temperature Plasma Diagnostics 2 Conference Tucson, Arizona June 19 22, 2 134 /KHB/wj ROLE OF DIAGNOSTICS IN ADVANCED TOKAMAK
More informationStudies of Turbulence and Transport in Alcator C- Mod H-Mode Plasmas with Phase Contrast Imaging and Comparisons with GYRO*
Studies of Turbulence and Transport in C- Mod H-Mode Plasmas with Phase Contrast Imaging and Comparisons with GYRO* M. Porkolab 1, L. Lin 1, E.M. Edlund 1, J.C. Rost 1, C.L. Fiore 1, M. Greenwald 1, Y.
More informationEdge Rotational Shear Requirements for the Edge Harmonic Oscillation in DIII D Quiescent H mode Plasmas
Edge Rotational Shear Requirements for the Edge Harmonic Oscillation in DIII D Quiescent H mode Plasmas by T.M. Wilks 1 with A. Garofalo 2, K.H. Burrell 2, Xi. Chen 2, P.H. Diamond 3, Z.B. Guo 3, X. Xu
More informationTRANSPORT PROGRAM C-MOD 5 YEAR REVIEW MAY, 2003 PRESENTED BY MARTIN GREENWALD MIT PLASMA SCIENCE & FUSION CENTER
TRANSPORT PROGRAM C-Mod C-MOD 5 YEAR REVIEW MAY, 2003 PRESENTED BY MARTIN GREENWALD MIT PLASMA SCIENCE & FUSION CENTER C-MOD - OPPORTUNITIES AND CHALLENGES Prediction and control are the ultimate goals
More informationEffects of drag and diffusion on nonlinear behavior of EP-driven instabilities.
IAEA-TM EP 2011 / 09 / 07 Effects of drag and diffusion on nonlinear behavior of EP-driven instabilities. Maxime Lesur Y. Idomura, X. Garbet, P. Diamond, Y. Todo, K. Shinohara, F. Zonca, S. Pinches, M.
More informationDynamics of Zonal Shear Collapse in Hydrodynamic Electron Limit. Transport Physics of the Density Limit
Dynamics of Zonal Shear Collapse in Hydrodynamic Electron Limit Transport Physics of the Density Limit R. Hajjar, P. H. Diamond, M. Malkov This research was supported by the U.S. Department of Energy,
More informationModeling of ELM Dynamics for ITER
Modeling of ELM Dynamics for ITER A.Y. PANKIN 1, G. BATEMAN 1, D.P. BRENNAN 2, A.H. KRITZ 1, S. KRUGER 3, P.B. SNYDER 4 and the NIMROD team 1 Lehigh University, 16 Memorial Drive East, Bethlehem, PA 18015
More informationCo-existence and interference of multiple modes in plasma turbulence: Some recent GENE results
Co-existence and interference of multiple modes in plasma turbulence: Some recent GENE results Frank Jenko IPP Garching, Germany University of Ulm, Germany Acknowledgements: F. Merz, T. Görler, D. Told,
More informationCharacteristics of Energetic-Ion-Driven Geodesic Acoustic Modes in the Large Helical Device(LHD)
O-4 12 th IAEA TM on Energetic Particles in Magnetic Confinement Systems, 7-10 Sep, Austin, USA Characteristics of Energetic-Ion-Driven Geodesic Acoustic Modes in the Large Helical Device(LHD) K. Toi,
More informationValidating Simulations of Multi-Scale Plasma Turbulence in ITER-Relevant, Alcator C-Mod Plasmas
Validating Simulations of Multi-Scale Plasma Turbulence in ITER-Relevant, Alcator C-Mod Plasmas Nathan Howard 1 with C. Holland 2, A.E. White 1, M. Greenwald 1, J. Candy 3, P. Rodriguez- Fernandez 1, and
More informationGyrokinetic neoclassical study of the bootstrap current in the tokamak edge pedestal with fully non-linear Coulomb collisions
Physics of Plasmas Gyrokinetic neoclassical study of the bootstrap current in the tokamak edge pedestal with fully non-linear Coulomb collisions Robert Hager 1, a) 1, b) and C.S. Chang Princeton Plasma
More informationC-Mod Core Transport Program. Presented by Martin Greenwald C-Mod PAC Feb. 6-8, 2008 MIT Plasma Science & Fusion Center
C-Mod Core Transport Program Presented by Martin Greenwald C-Mod PAC Feb. 6-8, 2008 MIT Plasma Science & Fusion Center Practical Motivations for Transport Research Overall plasma behavior must be robustly
More informationOn the Physics of Intrinsic Flow in Plasmas Without Magnetic Shear
On the Physics of Intrinsic Flow in Plasmas Without Magnetic Shear J. C. Li, R. Hong, P. H. Diamond, G. R. Tynan, S. C. Thakur, X. Q. Xu Acknowledgment: This material is based upon work supported by the
More informationIntrinsic rotation due to non- Maxwellian equilibria in tokamak plasmas. Jungpyo (J.P.) Lee (Part 1) Michael Barnes (Part 2) Felix I.
Intrinsic rotation due to non- Maxwellian equilibria in tokamak plasmas Jungpyo (J.P.) Lee (Part 1) Michael Barnes (Part 2) Felix I. Parra MIT Plasma Science & Fusion Center. 1 Outlines Introduction to
More informationA THEORETICAL AND EXPERIMENTAL INVESTIGATION INTO ENERGY TRANSPORT IN HIGH TEMPERATURE TOKAMAK PLASMAS
A THEORETICAL AND EXPERIMENTAL INVESTIGATION INTO ENERGY TRANSPORT IN HIGH TEMPERATURE TOKAMAK PLASMAS Presented by D.P. SCHISSEL Presented to APS Centennial Meeting March 20 26, 1999 Atlanta, Georgia
More informationImpact of neutral atoms on plasma turbulence in the tokamak edge region
Impact of neutral atoms on plasma turbulence in the tokamak edge region C. Wersal P. Ricci, F.D. Halpern, R. Jorge, J. Morales, P. Paruta, F. Riva Theory of Fusion Plasmas Joint Varenna-Lausanne International
More informationEnergetic-Ion-Driven MHD Instab. & Transport: Simulation Methods, V&V and Predictions
Energetic-Ion-Driven MHD Instab. & Transport: Simulation Methods, V&V and Predictions 7th APTWG Intl. Conference 5-8 June 2017 Nagoya Univ., Nagoya, Japan Andreas Bierwage, Yasushi Todo 14.1MeV 10 kev
More informationMHD-particle simulations and collective alpha-particle transport: analysis of ITER scenarios and perspectives for integrated modelling
MHD-particle simulations and collective alpha-particle transport: analysis of ITER scenarios and perspectives for integrated modelling G. Vlad, S. Briguglio, G. Fogaccia, F. Zonca Associazione Euratom-ENEA
More informationLow-collisionality density-peaking in GYRO simulations of C-Mod plasmas
Low-collisionality density-peaking in GYRO simulations of C-Mod plasmas D. R. Mikkelsen, M. Bitter, K. Hill, PPPL M. Greenwald, J.W. Hughes, J. Rice, MIT J. Candy, R. Waltz, General Atomics APS Division
More informationCoupled radius-energy turbulent transport of alpha particles
Coupled radius-energy turbulent transport of alpha particles George Wilkie, Matt Landreman, Ian Abel, William Dorland 24 July 2015 Plasma kinetics working group WPI, Vienna Wilkie (Maryland) Coupled transport
More informationNon-local Heat Transport in Alcator C-Mod Ohmic L-mode Plasmas
Non-local Heat Transport in Alcator C-Mod Ohmic L-mode Plasmas C. Gao 1, J.E.Rice 1, H.J. Sun 2,3, M.L.Reinke 1, N.T.Howard 1, D. Mikkelson 4, A.E.Hubbard 1, M.Chilenski 1, J.R.Walk 1, J.W.Hughes 1, P.Ennever
More informationSelf-consistent particle tracking in a simulation of the entropy mode in a Z pinch
Self-consistent particle tracking in a simulation of the entropy mode in a Z pinch K. Gustafson, I. Broemstrup, D. del-castillo-negrete, W. Dorland and M. Barnes Department of Physics, CSCAMM, University
More informationL Aquila, Maggio 2002
Nonlinear saturation of Shear Alfvén Modes and energetic ion transports in Tokamak equilibria with hollow-q profiles G. Vlad, S. Briguglio, F. Zonca, G. Fogaccia Associazione Euratom-ENEA sulla Fusione,
More informationTransport and turbulence reduction with negative triangularity : Correlation ECE measurements in TCV
Transport and turbulence reduction with negative triangularity : Correlation ECE measurements in TCV A. Pochelon, M.Rancic, V.S.Udintsev 1, T.P.Goodman, E.Fable 2, B.Labit, O.Sauter, R.Behn, A.Bottino
More informationKinetic damping in gyro-kinetic simulation and the role in multi-scale turbulence
2013 US-Japan JIFT workshop on New Aspects of Plasmas Kinetic Simulation NIFS, November 22-23, 2013 Kinetic damping in gyro-kinetic simulation and the role in multi-scale turbulence cf. Revisit for Landau
More informationGyrokine.c Analysis of the Linear Ohmic Confinement Regime in Alcator C- Mod *
Gyrokine.c Analysis of the Linear Ohmic Confinement Regime in Alcator C- Mod * Miklos Porkolab in collabora.on with J. Dorris, P. Ennever, D. Ernst, C. Fiore, M. Greenwald, A. Hubbard, E. Marmar, Y. Ma,
More informationDensity Peaking At Low Collisionality on Alcator C-Mod
Density Peaking At Low Collisionality on Alcator C-Mod APS-DPP Meeting Philadelphia, 10/31/2006 M. Greenwald, D. Ernst, A. Hubbard, J.W. Hughes, Y. Lin, J. Terry, S. Wukitch, K. Zhurovich, Alcator Group
More informationReduced Electron Thermal Transport in Low Collisionality H-mode Plasmas in DIII-D and the Importance of Small-scale Turbulence
1 Reduced Electron Thermal Transport in Low Collisionality H-mode Plasmas in DIII-D and the Importance of Small-scale Turbulence L. Schmitz, 1 C. Holland, 2 T.L. Rhodes, 1 G. Wang, 1 L. Zeng, 1 A.E. White,
More informationGA A THERMAL ION ORBIT LOSS AND RADIAL ELECTRIC FIELD IN DIII-D by J.S. degrassie, J.A. BOEDO, B.A. GRIERSON, and R.J.
GA A27822 THERMAL ION ORBIT LOSS AND RADIAL ELECTRIC FIELD IN DIII-D by J.S. degrassie, J.A. BOEDO, B.A. GRIERSON, and R.J. GROEBNER JUNE 2014 DISCLAIMER This report was prepared as an account of work
More informationITER Predictions Using the GYRO Verified and Experimentally Validated TGLF Transport Model
1 THC/3-3 ITER Predictions Using the GYRO Verified and Experimentally Validated TGLF Transport Model J.E. Kinsey, G.M. Staebler, J. Candy, and R.E. Waltz General Atomics, P.O. Box 8608, San Diego, California
More informationin tokamak plasmas Istvan Pusztai 1 Jeff Candy 2 Punit Gohil 2
Isotope mass and charge effects in tokamak plasmas Istvan Pusztai 1 Jeff Candy 2 Punit Gohil 2 (1) Chalmers University of Technology, Applied Physics, SE-412 96, Göteborg, Sweden (2) General Atomics, P.O.
More informationFormation and Back Transition of Internal Transport Barrier in Reversed Shear Plasmas
Formation and Back Transition of Internal Transport Barrier in Reversed Shear Plasmas S. S. Kim [1], Hogun Jhang [1], P. H. Diamond [1,2], [1] WCI Center for Fusion Theory, NFRI [2] CMTFO and CASS, UCSD,
More informationPSFC/JA D.R. Ernst, N. Basse, W. Dorland 1, C.L. Fiore, L. Lin, A. Long 2, M. Porkolab, K. Zeller, K. Zhurovich. June 2006
PSFC/JA-6-34 Identification of TEM Turbulence through Direct Comparison of Nonlinear Gyrokinetic Simulations with Phase Contrast Imaging Density Fluctuation Measurements D.R. Ernst, N. Basse, W. Dorland
More informationL-H Transition Dynamics and Power Threshold Minimum
L-H Transition Dynamics and Power Threshold Minimum M.A. Malkov 1, P.H. Diamond 1,2, K. Miki 2,3 and G.R. Tynan 1 1 University of California, San Diego, USA; e-mail: mmalkov@ucsd.edu 2 WCI, NFRI Daejeon,
More informationProgress of Full- f Gyrokinetic Simulation Toward Reactor Relevant Numerical Experiments )
Progress of Full- f Gyrokinetic Simulation Toward Reactor Relevant Numerical Experiments ) Yasuhiro IDOMURA, Motoki NAKATA 1) and Sébastien JOLLIET 2) Japan Atomic Energy Agency, Kashiwanoha, 5-1-5 Kashiwa,
More informationSimulation of alpha particle current drive and heating in spherical tokamaks
Simulation of alpha particle current drive and heating in spherical tokamaks R. Farengo 1, M. Zarco 1, H. E. Ferrari 1, 1 Centro Atómico Bariloche and Instituto Balseiro, Argentina. Consejo Nacional de
More informationIntrinsic Rotation and Toroidal Momentum Transport: Status and Prospects (A Largely Theoretical Perspective)
Intrinsic Rotation and Toroidal Momentum Transport: Status and Prospects (A Largely Theoretical Perspective) P.H. Diamond [1] WCI Center for Fusion Theory, NFRI, Korea [2] CMTFO and CASS, UCSD, USA Thought
More informationTurbulence spreading and transport scaling in global gyrokinetic particle simulations
PHYSICS OF PLASMAS VOLUME 11, NUMBER 3 MARCH 2004 Turbulence spreading and transport scaling in global gyrokinetic particle simulations Z. Lin Department of Physics and Astronomy, University of California,
More informationInfluence of Beta, Shape and Rotation on the H-mode Pedestal Height
Influence of Beta, Shape and Rotation on the H-mode Pedestal Height by A.W. Leonard with R.J. Groebner, T.H. Osborne, and P.B. Snyder Presented at Forty-Ninth APS Meeting of the Division of Plasma Physics
More informationECH Density Pumpout and Small Scale Turbulence in DIII-D
ECH Density Pumpout and Small Scale Turbulence in DIII-D By K.L. Wong, T.L. Rhodes, R. Prater, R. Jayakumar, R. Budny, C.C. Petty, R. Nazikian, and W.A. Peebles Background It has been known for more than
More informationLocal gyrokinetic turbulence simulations with realistic tokamak geometries towards ITER and JT-60SA
Local gyrokinetic turbulence simulations with realistic tokamak geometries towards ITER and JT-6SA M. Nakata, A. Matsuyama, N. Aiba, S. Maeyama in collaboration with T. -H. Watanabe, H. Sugama, and M.
More informationMinimal Model Study for ELM Control by Supersonic Molecular Beam Injection and Pellet Injection
25 th Fusion Energy Conference, Saint Petersburg, Russia, 2014 TH/P2-9 Minimal Model Study for ELM Control by Supersonic Molecular Beam Injection and Pellet Injection Tongnyeol Rhee 1,2, J.M. Kwon 1, P.H.
More informationS. Ku 1, C.S. Chang 1,2, and P.H. Diamond 3. New York University, NY 10012, USA. Daejon, Republic of Korea and
Full-f gyrokinetic particle simulation of centrally heated global ITG turbulence from magnetic axis to edge pedestal top in a realistic tokamak geometry S. Ku 1, C.S. Chang 1,2, and P.H. Diamond 3 1 Courant
More informationDPG School The Physics of ITER Physikzentrum Bad Honnef, Energy Transport, Theory (and Experiment) Clemente Angioni
Max-Planck-Institut für Plasmaphysik DPG School The Physics of ITER Physikzentrum Bad Honnef, 23.09.2014 Energy Transport, Theory (and Experiment) Clemente Angioni Special acknowledgments for material
More informationIntegrated Heat Transport Simulation of High Ion Temperature Plasma of LHD
1 TH/P6-38 Integrated Heat Transport Simulation of High Ion Temperature Plasma of LHD S. Murakami 1, H. Yamaguchi 1, A. Sakai 1, K. Nagaoka 2, H. Takahashi 2, H. Nakano 2, M. Osakabe 2, K. Ida 2, M. Yoshinuma
More informationEnergetic particle modes: from bump on tail to tokamak plasmas
Energetic particle modes: from bump on tail to tokamak plasmas M. K. Lilley 1 B. N. Breizman 2, S. E. Sharapov 3, S. D. Pinches 3 1 Physics Department, Imperial College London, London, SW7 2AZ, UK 2 IFS,
More informationCritical gradient formula for toroidal electron temperature gradient modes
PHYSICS OF PLASMAS VOLUME 8, NUMBER 9 SEPTEMBER 2001 Critical gradient formula for toroidal electron temperature gradient modes F. Jenko, W. Dorland, a) and G. W. Hammett b) Max-Planck-Institut für Plasmaphysik,
More informationInnovative Concepts Workshop Austin, Texas February 13-15, 2006
Don Spong Oak Ridge National Laboratory Acknowledgements: Jeff Harris, Hideo Sugama, Shin Nishimura, Andrew Ware, Steve Hirshman, Wayne Houlberg, Jim Lyon Innovative Concepts Workshop Austin, Texas February
More informationNon-local Heat Transport, Core Rotation Reversals and Energy Confinement Saturation in Alcator C-Mod Ohmic L-mode Plasmas
1 EX/2-2 Non-local Heat Transport, Core Rotation Reversals and Energy Confinement Saturation in Alcator C-Mod Ohmic L-mode Plasmas J.E. Rice 1, M.L. Reinke 1, H.J. Sun 2, P.H. Diamond 3,4, C. Gao 1, N.T.
More informationComparison of Critical Values of R/L Te. for ETG Modes Based on an Analytic Expression. with GKS Simulations for DIII-D Discharges
Comparison of Critical Values of R/L Te for ETG Modes Based on an Analytic Expression with GKS Simulations for DIII-D Discharges J.C. DeBoo, D.R. Baker and G.M. Staebler DIII-D National Fusion Facility
More informationShear Flow Generation in Stellarators - Configurational Variations
Shear Flow Generation in Stellarators - Configurational Variations D. A. Spong 1), A. S. Ware 2), S. P. Hirshman 1), J. H. Harris 1), L. A. Berry 1) 1) Oak Ridge National Laboratory, Oak Ridge, Tennessee
More informationControl of Neo-classical tearing mode (NTM) in advanced scenarios
FIRST CHENGDU THEORY FESTIVAL Control of Neo-classical tearing mode (NTM) in advanced scenarios Zheng-Xiong Wang Dalian University of Technology (DLUT) Dalian, China Chengdu, China, 28 Aug, 2018 Outline
More informationOVERVIEW OF THE ALCATOR C-MOD PROGRAM. IAEA-FEC November, 2004 Alcator Team Presented by Martin Greenwald MIT Plasma Science & Fusion Center
OVERVIEW OF THE ALCATOR C-MOD PROGRAM IAEA-FEC November, 2004 Alcator Team Presented by Martin Greenwald MIT Plasma Science & Fusion Center OUTLINE C-Mod is compact, high field, high density, high power
More informationHybrid Kinetic-MHD simulations with NIMROD
simulations with NIMROD 1 Yasushi Todo 2, Dylan P. Brennan 3, Kwang-Il You 4, Jae-Chun Seol 4 and the NIMROD Team 1 University of Washington, Seattle 2 NIFS, Toki-Japan 3 University of Tulsa 4 NFRI, Daejeon-Korea
More informationStability of a plasma confined in a dipole field
PHYSICS OF PLASMAS VOLUME 5, NUMBER 10 OCTOBER 1998 Stability of a plasma confined in a dipole field Plasma Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139 Received
More informationFlow and dynamo measurements in the HIST double pulsing CHI experiment
Innovative Confinement Concepts (ICC) & US-Japan Compact Torus (CT) Plasma Workshop August 16-19, 211, Seattle, Washington HIST Flow and dynamo measurements in the HIST double pulsing CHI experiment M.
More informationW.A. HOULBERG Oak Ridge National Lab., Oak Ridge, TN USA. M.C. ZARNSTORFF Princeton Plasma Plasma Physics Lab., Princeton, NJ USA
INTRINSICALLY STEADY STATE TOKAMAKS K.C. SHAING, A.Y. AYDEMIR, R.D. HAZELTINE Institute for Fusion Studies, The University of Texas at Austin, Austin TX 78712 USA W.A. HOULBERG Oak Ridge National Lab.,
More informationIntroduction to Fusion Physics
Introduction to Fusion Physics Hartmut Zohm Max-Planck-Institut für Plasmaphysik 85748 Garching DPG Advanced Physics School The Physics of ITER Bad Honnef, 22.09.2014 Energy from nuclear fusion Reduction
More informationEffects of Alpha Particle Transport Driven by Alfvénic Instabilities on Proposed Burning Plasma Scenarios on ITER
Effects of Alpha Particle Transport Driven by Alfvénic Instabilities on Proposed Burning Plasma Scenarios on ITER G. Vlad, S. Briguglio, G. Fogaccia, F. Zonca Associazione Euratom-ENEA sulla Fusione, C.R.
More information