Stable TAE n Discrimination with Plasma Rotation

Slides:



Advertisements
Similar presentations
Control of Magnetic Chaos & Self-Organization John Sarff for MST Group CMSO General Meeting Madison, WI August 4-6, 2004.
Advertisements

Ideas for overseas contributions to CMSO Piero Martin Consorzio RFX Associazione Euratom-ENEA sulla fusione And Physics Dept., Univ. of Padova, Italy CMSO.
Dynamical plasma response during driven magnetic reconnection in the laboratory Ambrogio Fasoli* Jan Egedal MIT Physics Dpt & Plasma Science and Fusion.
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.
INTRODUCTION OF WAVE-PARTICLE RESONANCE IN TOKAMAKS J.Q. Dong Southwestern Institute of Physics Chengdu, China International School on Plasma Turbulence.
Discrete Alfven Eigenmodes Shuang-hui Hu College of Sci, Guizhou Univ, Guiyang Liu Chen Dept of Phys & Astr, UC Irvine Supported by DOE and NSF.
Faculty of Science Department of Physics Field Line Resonances in the Earth’s Magnetosphere and Astrophysical Plasmas 1 J. C. Samson
Progress of Alfven wave experiment in SUNIST The 2 nd A3 Foresight Workshop on Spherical Torus, January, 2014, Beijing, China Y. Tan 1*, Z. Gao 1,
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.
“Three-D MHD numerical simulations of coronal loop oscillations associated with flares” Miyagoshi et al., PASJ 56, 207, 2004.
T. Hellsten IEA Burning Plasma Workshop, July 2005 Tarragona Spain Integrated Modelling of ICRH and AE Dynamics T. Hellsten, T. Bergkvist, T. Johnson and.
Nils P. Basse Plasma Science and Fusion Center Massachusetts Institute of Technology Cambridge, MA USA ABB seminar November 7th, 2005 Measurements.
Reflectometry on Alcator C-Mod: Status and future upgrades Outline: C-Mod reflectometry Physics examples Upgrades: 1.High frequency 2.Sideband 3.Data acquisition.
NSTX S. A. Sabbagh XP501: MHD spectroscopy of wall stabilized high  plasmas  Motivation  Resonant field amplification (RFA) observed in high  NSTX.
Nonlinear Frequency Chirping of Alfven Eigenmode in Toroidal Plasmas Huasen Zhang 1,2 1 Fusion Simulation Center, Peking University, Beijing , China.
J A Snipes, 6 th ITPA MHD Topical Group Meeting, Tarragona, Spain 4 – 6 July 2005 TAE Damping Rates on Alcator C-Mod Compared with Nova-K J A Snipes *,
H-mode characteristics close to L-H threshold power ITPA T&C and Pedestal meeting, October 09, Princeton Yves Martin 1, M.Greenwald, A.Hubbard, J.Hughes,
Hybrid Simulations of Energetic Particle-driven Instabilities in Toroidal Plasmas Guo-Yong Fu In collaboration with J. Breslau, J. Chen, E. Fredrickson,
TH/7-2 Radial Localization of Alfven Eigenmodes and Zonal Field Generation Z. Lin University of California, Irvine Fusion Simulation Center, Peking University.
The Role of Damping in Stable and Unstable Alfvén Eigenmodes S. D. Pinches 1, A. Könies 2, Ph. Lauber 1 H.L.Berk 3, S.E.Sharapov 4 and M.Gryaznavich 4.
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.
HAGIS Code Lynton Appel … on behalf of Simon Pinches and the HAGIS users CCFE is the fusion research arm of the United Kingdom Atomic Energy Authority.
Characterization of core and edge turbulence in L- and H-mode Alcator C-Mod plasmas Outline: Alcator C-Mod tokamak Fluctuation diagnostics Low to high.
1 Confinement Studies on TJ-II Stellarator with OH Induced Current F. Castejón, D. López-Bruna, T. Estrada, J. Romero and E. Ascasíbar Laboratorio Nacional.
Investigation of fast ion mode spatial structure in NSTX N.A. Crocker, S. Kubota, W.A. Peebles (UCLA); E.D. Fredrickson, N.N. Gorelenkov, G.J. Kramer,
Study of NSTX Electron Density and Magnetic Field Fluctuation using the FIReTIP System K.C. Lee, C.W. Domier, M. Johnson, N.C. Luhmann, Jr. University.
MHD Suppression with Modulated LHW on HT-7 Superconducting Tokamak* Support by National Natural Science Fund of China No J.S.Mao, J.R.Luo, B.Shen,
Measurement of toroidal rotation velocity profiles in KSTAR S. G. Lee, Y. J. Shi, J. W. Yoo, J. Seol, J. G. Bak, Y. U. Nam, Y. S. Kim, M. Bitter, K. Hill.
S. Coda, MHD workshop, PPPL, 22 Nov Advances in sawtooth control for NTM prevention in JET S. Coda 1, L.-G. Eriksson 2, J. Graves 1, R. Koslowski.
1 Stability Studies Plans (FY11) E. Fredrickson, For the NCSX Team NCSX Research Forum Dec. 7, 2006 NCSX.
The Infrared Spectrum of CH 5 + Revisited Kyle N. Crabtree, James N. Hodges, and Benjamin J. McCall.
Alfven Waves in Toroidal Plasmas
Enhanced D  H-mode on Alcator C-Mod presented by J A Snipes with major contributions from M Greenwald, A E Hubbard, D Mossessian, and the Alcator C-Mod.
T. Hellsten IAEA TM Meeting on Energetic Particles, San Diego 2003 T. Hellsten 1, T. Bergkvist 1, T.Johnson 1, M. Laxåback 1 and L.-G. Eriksson 2 1 Euratom-VR.
Nonlinear Simulations of Energetic Particle-driven Modes in Tokamaks Guoyong Fu Princeton Plasma Physics Laboratory Princeton, NJ, USA In collaboration.
NSTX SAS – GMS Mtg. 12/1/04 S. A. Sabbagh and J. E. Menard NSTX RWM Active Feedback System Implementation Plan Discussion NSTX Global Mode Stabilization.
NSTX S. A. Sabbagh XP452: RWM physics with initial global mode stabilization coil operation  Goals  Alter toroidal rotation / examine critical rotation.
Current Drive Experiments with Oscillating Toroidal Flux in HT-7 Superconducting Tokamak J.S.Mao, P. Phillips 1, J.R.Luo, J.Y.Zhao, Q.L.Wu, Z.W.Wu, J.G.Li,
NSTX S. A. Sabbagh XP407: Passive Stabilization Physics of the RWM in High  N ST Plasmas – 4/13/04  Goals  Define RWM stability boundary in (V , 
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.
6 th ITPA MHD Topical Group Meeting combined with W60 IEA Workshop on Burning Plasmas Summary Session II MHD Stability and Fast Particle Confinement chaired.
Turbulence associated with the control of internal transport barriers
8th IAEA Technical Meeting on
C.K. Phillips, J. Hosea, E. Valeo, J.R. Wilson PPPL
Garching-Greifswald Ringberg Theory Meeting
Two new tools at Alcator C-Mod yield fundamental insights into short-, coherent edge fluctuations associated with steady-state, reactor-relevant regimes.
Generation of Toroidal Rotation by Gas Puffing
Impact of a Mock-up Ferromagnetic TBM on Plasma Operations in C-Mod
MHD Induced Fast Ion Loss Diagnostic for Alcator C-Mod
משרד התעשייה, המסחר והתעסוקה פעולות המשרד לעידוד מגזר המיעוטים
Does quasi-coherent mode limit pedestal pressure gradient?
R. Granetz1, S. Wolfe1, D. Whyte1, V. Izzo1, M. Reinke1, J. Terry1, A
Advanced Scenarios: ITER-like Hybrid at Low Bt without LH
Comparisons of Measurements and Gyro-kinetic Simulations of Turbulence and Trans-port in Alcator C-Mod EDA H-Mode Discharges M. B. Sampsell, R. V. Bravenec.
Visible Doppler Spectrometer for Edge Toroidal Rotation
TC-2 – Power ratio April 2011, San Diego
Determining confinement and stability of q(0)>1 regimes produced
ITB Control with LH Heating & Current Drive
Study of Fast Ions in CESR
Experimental Plan for the New Wall-Actuated Scanning Probe (WASP)
NTM Stability at Low Collisionality
ITER ICRF Scenario Demonstration in Hydrogen with 3He Minority Heating
Ballooning Structure of Core Turbulence
Stabilization of m/n=1/1 fishbone by ECRH
NATIONAL RESEARCH CENTER “KURCHATOV INSTITUTE”
Alfven Oscillations in the TUMAN-3M Tokamak Ohmic Regime
Electron Acoustic Waves in Pure Ion Plasmas F. Anderegg C. F
LoHCo Meeting – Tucson, December 13, 2005
Reflectometry measurements of turbulence in Alcator C-Mod plasmas
Self-organization to Stable magnetic Plasmas by
Presentation transcript:

Stable TAE n Discrimination with Plasma Rotation J. A. Snipes, A. Fasoli*, J. E. Rice, J. A. Sears MIT Plasma Science and Fusion Center, Cambridge, MA USA *CRPP-EPFL Association Euratom, Lausanne, Switzerland J A Snipes, Alcator C-Mod Ideas Forum, MIT PSFC, Cambridge, MA 13 – 15 December 2006

Improved Toroidal Mode Number Measurements New pick-up coil limiters at four toroidal locations will improve low n resolution for all MHD modes  If multiple n’s are simultaneously excited by the TAE antennas, a large plasma rotation should separate the modes in frequency J A Snipes, Alcator C-Mod Ideas Forum, MIT PSFC, Cambridge, MA 13 – 15 December 2006

Plasma Rotation in Ohmic H-mode Reaches 40 km/s ~ 9.5 kHz Motivation: Actively excited TAE measured phases often show no clear n number. The broad antenna spectrum may excite multiple n’s simultaneously. Knowing n is essential to compare with theory. Goals: Excite stable TAEs with the active MHD antennas during high plasma rotation • Look for closely frequency spaced multiple n modes with spacing proportional to plasma rotation • Attempt to discriminate the various n values and determine the damping rate as a function of n • Compare high n damping rate with theoretical expectation of increased radiative damping at high n Plan of execution: In Ohmic H-mode plasmas: • Sweep active MHD antenna frequency through the real-time TAE frequency and look for resonances • Attempt to maximize plasma rotation in H-mode • Look for frequency splitting of each resonance • Sweep through frequencies associated with high n>10 to attempt to drive higher n modes J E Rice, et al, 2004 Phys Plasmas 11, 2427 J A Snipes, Alcator C-Mod Ideas Forum, MIT PSFC, Cambridge, MA 13 – 15 December 2006