Edge Zonal Flows and Blob Propagation in Alcator C-Mod P5.073 EPS 2011

Size: px
Start display at page:

Download "Edge Zonal Flows and Blob Propagation in Alcator C-Mod P5.073 EPS 2011"

Transcription

1 Edge Zonal Flows and Blob Propagation in Alcator C-Mod S.J. Zweben 1, J.L. Terry 2, M. Agostini 3, B. Davis 1, O. Grulke 4,J. Hughes 2, B. LaBombard 2 D.A. D'Ippolito 6, R. Hager 5, J.R. Myra 6, D.A. Russell 6 1 Princeton Plasma Physics Laboratory, Princeton NJ Massachusetts Institute of Technology, Cambridge MA Consorzio RFX, Associazione EURATOM, I-35127, Padova Italy 4 Max Planck Institute for Plasma Physics, D-17489, Greifswald, Germany 5 Max Planck Institute for Plasma Physics, D Garching, Germany 6 Lodestar Research Corporation, 2400 Central Ave., Boulder CO P5.073 EPS

2 Outline of this Poster Motivations GPI diagnostic Edge zonal flows Blob propagation Further directions 2

3 Motivations for Studying Zonal Flows Radial turbulence velocity is probably the main cause of radial transport in the edge and SOL Poloidal turbulence velocity can reduce radial transport by suppressing or shearing turbulent structures Big issue at present is whether steady mean flow or fluctuating zonal flow is more important Prior mean turbulence velocity measurements in C-Mod: - Velocity fields from PSI-5 GPI camera (Terry, J. Nucl. Mat 2005) - Radial velocity from probe ExB (Smick & LaBombard, RSI 2009) - Blob radial and poloidal velocity (Grulke, PoP 2006) - Poloidal velocity from APD array (Cziegler, POP 2010) - Radial velocity from Phantom 7.3 GPI camera (Zweben, JNM 2010) - Velocity fields vs. density (Agostini, Nucl. Fus. 2011) 3

4 Motivations for Studying Blob Motion Try to clarify mechanism of blob formation, i.e. where and why are blobs formed Compare radial motion of blobs to theory and simulation to better understand their effect on the SOL width Compare blob velocities to velocities derived from crosscorrelation technique Prior blob motion measurements on C-Mod: - Blob radial velocity from GPI-probe correlations (Grulke, PoP 2006) - Blob radial velocity vs. analytic blob models (Zweben, JNM 2010) - blob birth and radial speed vs. density (Agostini, Nucl. Fus. 2011) 4

5 Gas Puff Imaging Diagnostic GPI view using Phantom 710 camera data at 400,000 frames/sec select shots with good B-field alignment q 95 ~ 3.4 ± 0.4 select shots with good gas puff contrast (both D and He) => 30 shots in the database for this poster 5

6 Interpreta(on of GPI- Inferred Velocity GPI views local emission of D α ~ n o f(n e,t e ) within window where D α is emitted in plasma edge, where T e ~ ev Can measure 2-D turbulence structure and motion even if response of D α is nonlinear (like contrast knob on a TV) Can not directly measure fluid (ion) flow or ExB flow, but measures turbulence or blob velocity, as done previously in studies of edge zonal flow * * McKee et al, PoP 03 using BES on DIII-D Conway et al, PPCF 05 using Doppler reflectometry on AUG 6 6

7 Examples of GPI Camera Images raw data first normalized to a time-averaged frame movies can be seen at CMod2010/CMod2010.html MA, 3.6 T no RF MA, 5.3 T 1.6 MW RF 7 7

8 Zonal Flow Algorithm one frame 6 cm poloidal 6 cm radial (outward) - for each pixel in each frame, make a short time series of the GPI signal at that pixel over ±5 frames or ~25 µs total - find best match to this time series in pixels of the next frame and get V rad and V pol from displacement to best match - average 4 cm poloidally to get zonal flow velocity 8 8

9 Cross-Correlation Analysis Outputs Finds time-resolved, poloidally-averaged velocities vs. radius V pol frequency response ~30 khz (1/e of amplitude at f~0) V pol and V rad vs. time at ρ=0.3 cm frequency response 9

10 Spatial Variation of Poloidal Velocity Significant poloidal variation of V pol in all cases, thus the poloidal average of V pol is not just an m=0 zonal flow Radial profile of (poloidally averaged) V pol shows timeaveraged structure which varies slowly with radius 10

11 Mean Velocities vs. Radius Poloidal velocities vary considerably, but generally in IDD Radial velocities outward in SOL but slightly negative inside separatrix (similar to Terry JNM 05 and Agostini NF 11) V pol vs. radius V rad vs. radius 11

12 Spectra of Velocity Fluctuations Radial velocity Poloidal velocity MA, 3.6 T ρ= cm P rf = MA, 5.3 T ρ= cm P rf = 1.6 MW 12

13 Velocity Spectra vs. Radius vs. Time Radial velocity Poloidal velocity MA, 3.6 T ρ= cm P rf = MA, 5.3 T ρ= cm P rf = 1.6 MW 13

14 Correlation of Velocity and MHD Shots with incoherent (broadband) spectra of V pol do not have a clear correlation of V pol & MHD Shots with a clear coherent spectra of V pol have a partial correlation of V pol & MHD (e.g. at 6.5 khz in ) 14 (thanks to David Pace for help with InSpect)

15 Theoretical GAM Frequency for C-Mod GAM frequency f = G c s /(πr) with G=geometric factor, R = R o +r, and c s = [γ(t i +T e )/m i ] 1/2 where G~ (2-1/2 ) (2/(1+κ) (1+1/(2A 2/3 ) (1+1/(4q 2 )) For C-Mod with A=3, κ=1.6, q=3, T e =T i =50 ev, γ=4/3 and m i =2 f GAM ~ 20 khz These analytic values (from R. Hager) can still deviate a factor-of-two from experiment (Hallatschek PPCF 2007, Conway PPCF 2008) 15

16 L-H Transition and ELMs Coherent V pol at ~ 6.5 khz disappears at L-H transition Both V pol and V rad increase transiently at ELMs V sec sec Time (sec) 16

17 Radial Correlation of V pol Fluctuations Find maximum of <V pol (r,t) V pol (r,t) > at (r -r) = 0.35 cm Increased poloidal velocity correlation at lower <n e > 17

18 Are These Zonal Flows? Poloidal correlation of V pol over GPI view in poloidal angle (~ 5 L pol ) and radius (~ 1 L rad ) is a fairly good indicator of zonal flow (similar to BES and single-ch. reflectometry) Frequency range of V pol fluctuations similar to other zonal flow fluctuations (e.g khz in DIII-D, 3 khz in NSTX) Amplitude of V pol fluctuations is comparable to mean flows, similar zonal flows to other devices (e.g. AUG) Magnetic component may be from EGAM or zonal field => Tentative answer is yes 18

19 Blob Motion Algorithm In normalized images, find regions with closed contours Define blob as any region above 1.2 normalized value Track blob centers over time to determine blob velocity Blob motion over µs/frame (# ) 19

20 Examples of Blob Tracking Blob center trajectories calculated over time in all images Proximity criteria set to insure continuity of blob motion blob tracks starting within radial box over 2 msec period vertical pixel vertical pixel horizontal pixel horizontal pixel 20

21 Distribution of Radial Blob Speeds Radial speed distribution of blobs is broad at all radii in SOL Not much variation in speeds over ρ = cm in this case Blob speed similar to Grulke POP (2006), Agostini (NF 2011) 21

22 Cross-Correlation vs. Blob Velocity averaged over 20 msec (error bars are velocity fluctuations) comparison with velocity codes of M. Agostini in progresss 22

23 Some Open Issues (Experimental) Look for global correlation of δv pol with other diagnostics Look at correlations <δv pol δv rad > for Reynolds stress Look at correlations <δv pol δi GPI > for transport effects Evaluate poloidal m-spectrum of δv pol within GPI box Reconcile poloidal flows with poloidal phase speeds Look at shots in H-mode and with various types of MHD Cross-correlate δv pol and MHD vs. poloidal angle Look for scaling of blob speed with SOL parameters 23

24 Some Open Issues (Theoretical) Compare with expected frequency of GAMs and EGAMs Compare with zonal flows in SOLT calculation (Lodestar) Evaluate effect of collisional damping on edge zonal flow Understand physics of zonal flows on open field lines Evaluate edge poloidal flows expected for MHD modes Evaluate whether magnetic zonal fields are expected Compare blob speed distributions with blob theory Compare blob formation process with blob theory 24

Blob sizes and velocities in the Alcator C-Mod scrapeoff

Blob sizes and velocities in the Alcator C-Mod scrapeoff P1-59 Blob sizes and velocities in the Alcator C-Mod scrapeoff layer R. Kube a,b,*, O. E. Garcia a,b, B. LaBombard b, J. L. Terry b, S. J. Zweben c a Department of Physics and Technology, University of

More information

Varia%ons in Edge and SOL Turbulence in NSTX

Varia%ons in Edge and SOL Turbulence in NSTX Varia%ons in Edge and SOL Turbulence in NSTX S.J. Zweben 1*, W.M. Davis 1, S.M. Kaye 1, J.R. Myra 2, R.E. Bell 1, B.P LeBlanc 1, R.J. Maqueda 1**, T. Munsat 3, S.A. Sabbagh 4, Y. Sechrest 3, D.P. Stotler

More information

Connections between Particle Transport and Turbulence Structures in the Edge and SOL of Alcator C-Mod

Connections between Particle Transport and Turbulence Structures in the Edge and SOL of Alcator C-Mod Connections between Particle Transport and Turbulence Structures in the Edge and SOL of Alcator C-Mod I. Cziegler J.L. Terry, B. LaBombard, J.W. Hughes MIT - Plasma Science and Fusion Center th 19 Plasma

More information

Rapid changes of turbulence propagation direction in the edge of

Rapid changes of turbulence propagation direction in the edge of Rapid changes of turbulence propagation direction in the edge of I. Cziegler, J. L. Terry MIT Plasma Science and Fusion Center APS Division of Plasma Physics Dallas TX, November 8 Motivations for edge/sol

More information

Overview Impact of 3D fields (RMP) on edge turbulence and turbulent transport

Overview Impact of 3D fields (RMP) on edge turbulence and turbulent transport Trilateral Euregio Cluster Overview Impact of 3D fields (RMP) on edge turbulence and turbulent transport TEC Yuhong Xu Laboratory for Plasma Physics, Ecole Royale Militaire - Koninklijke Militaire School,

More information

Plasma Science and Fusion Center

Plasma Science and Fusion Center Plasma Science and Fusion Center Turbulence and transport studies in ALCATOR C Mod using Phase Contrast Imaging (PCI) Diagnos@cs and Comparison with TRANSP and Nonlinear Global GYRO Miklos Porkolab (in

More information

Blob motion and control. simple magnetized plasmas

Blob motion and control. simple magnetized plasmas Blob motion and control in simple magnetized plasmas Christian Theiler A. Fasoli, I. Furno, D. Iraji, B. Labit, P. Ricci, M. Spolaore 1, N. Vianello 1 Centre de Recherches en Physique des Plasmas (CRPP)

More information

Effect of divertor nitrogen seeding on the power exhaust channel width in Alcator C-Mod

Effect of divertor nitrogen seeding on the power exhaust channel width in Alcator C-Mod Effect of divertor nitrogen seeding on the power exhaust channel width in Alcator C-Mod B. LaBombard, D. Brunner, A.Q. Kuang, W. McCarthy, J.L. Terry and the Alcator Team Presented at the International

More information

The I-phase and its relation to other phenomena at AUG

The I-phase and its relation to other phenomena at AUG Max-Planck-Institut für Plasmaphysik The I-phase and its relation to other phenomena at AUG G. Birkenmeier, M. Cavedon, G.D. Conway, P. Manz, G. Fuchert, F. M. Laggner, T. Happel, A. Medvedeva, V. Nikolaeva,

More information

Experimental investigation of the parallel structure of fluctuations in the scrape-off layer of Alcator C-Mod

Experimental investigation of the parallel structure of fluctuations in the scrape-off layer of Alcator C-Mod Experimental investigation of the parallel structure of fluctuations in the scrape-off layer of Alcator C-Mod O. Grulke Max Planck Institute for Plasma Physics, Greifswald Branch, EURATOM Association,

More information

IF2011 Pedestal/JRT Summary. J.W. Hughes 21 Jan 2011

IF2011 Pedestal/JRT Summary. J.W. Hughes 21 Jan 2011 IF2011 Pedestal/JRT Summary J.W. Hughes 21 Jan 2011 Predictive capability for the H-mode pedestal is the subject of the FY11 JRT Statement of FY11 FES Joint Research Target: (1) Improve the understanding

More information

Spatial, temporal and spectral structure of the turbulence-flow interaction at the L-H transition

Spatial, temporal and spectral structure of the turbulence-flow interaction at the L-H transition Spatial, temporal and spectral structure of the turbulence-flow interaction at the L-H transition T Estrada 1, E. Ascasíbar 1, E. Blanco 1, A. Cappa 1, P. H. Diamond 2, T. Happel 3, C. Hidalgo 1, M. Liniers

More information

High Speed Imaging of Edge Turbulence in NSTX

High Speed Imaging of Edge Turbulence in NSTX High Speed Imaging of Edge Turbulence in NSTX S.J. Zweben, R. Maqueda 1, D.P. Stotler, A. Keesee 2, J. Boedo 3, C. Bush 4, S. Kaye, B. LeBlanc, J. Lowrance 5, V. Mastrocola 5, R. Maingi 4, N. Nishino 6,

More information

Nonlinear Evolution and Radial Propagation of the Energetic Particle Driven GAM

Nonlinear Evolution and Radial Propagation of the Energetic Particle Driven GAM Nonlinear Evolution and Radial Propagation of the Energetic Particle Driven GAM by R. Nazikian In collaboration with G.Y. Fu, R.V. Budny, G.J. Kramer, PPPL G.R. McKee, U. Wisconsin T. Rhodes, L. Schmidt,

More information

Modeling neutral-plasma interactions in scrape-off layer (SOLT) simulations*

Modeling neutral-plasma interactions in scrape-off layer (SOLT) simulations* Modeling neutral-plasma interactions in scrape-off layer (SOLT) simulations* D. A. Russell and J. R. Myra Research Corporation Boulder CO USA Presented at the US Transport Task Force Workshop Williamsburg

More information

Relating the L-H Power Threshold Scaling to Edge Turbulence Dynamics

Relating the L-H Power Threshold Scaling to Edge Turbulence Dynamics Relating the L-H Power Threshold Scaling to Edge Turbulence Dynamics Z. Yan 1, G.R. McKee 1, J.A. Boedo 2, D.L. Rudakov 2, P.H. Diamond 2, G. Tynan 2, R.J. Fonck 1, R.J. Groebner 3, T.H. Osborne 3, and

More information

Sensitivity of Tokamak Transport Modeling to Atomic Physics Data: Some Examples

Sensitivity of Tokamak Transport Modeling to Atomic Physics Data: Some Examples Sensitivity of Tokamak Transport Modeling to Atomic Physics Data: Some Examples, S. Baek, J. D. Elder, M. L. Reinke, F. Scotti, J. L. Terry, S. J. Zweben IAEA Technical Meeting on Uncertainty Assessment

More information

Scalings of nonlinearity in the edge plasma and its connection to transition thresholds

Scalings of nonlinearity in the edge plasma and its connection to transition thresholds Scalings of nonlinearity in the edge plasma and its connection to transition thresholds I. Cziegler, P. H. Diamond, G. R. Tynan UCSD, Center for Momentum Transport and Flow Organization A. E. Hubbard,

More information

Alcator C-Mod. Particle Transport in the Scrape-off Layer and Relationship to Discharge Density Limit in Alcator C-Mod

Alcator C-Mod. Particle Transport in the Scrape-off Layer and Relationship to Discharge Density Limit in Alcator C-Mod Alcator C-Mod Particle Transport in the Scrape-off Layer and Relationship to Discharge Density Limit in Alcator C-Mod B. LaBombard, R.L. Boivin, M. Greenwald, J. Hughes, B. Lipschultz, D. Mossessian, C.S.

More information

Partially Coherent Fluctuations in Novel High Confinement Regimes of a Tokamak

Partially Coherent Fluctuations in Novel High Confinement Regimes of a Tokamak Partially Coherent Fluctuations in Novel High Confinement Regimes of a Tokamak István Cziegler UCSD, Center for Energy Research Center for Momentum Transport and Flow Organization Columbia Seminar Feb

More information

Invited Review Article: Gas Puff Imaging Diagnostics of Edge Plasma Turbulence in Magnetic Fusion Devices. X Science LLC, Plainsboro, NJ 08536, USA

Invited Review Article: Gas Puff Imaging Diagnostics of Edge Plasma Turbulence in Magnetic Fusion Devices. X Science LLC, Plainsboro, NJ 08536, USA Invited Review Article: Gas Puff Imaging Diagnostics of Edge Plasma Turbulence in Magnetic Fusion Devices S.J. Zweben 1, J.L. Terry 2, D.P. Stotler 1, R.J. Maqueda 3 1 Princeton Plasma Physics Laboratory,

More information

Pedestals and Fluctuations in C-Mod Enhanced D α H-modes

Pedestals and Fluctuations in C-Mod Enhanced D α H-modes Pedestals and Fluctuations in Enhanced D α H-modes Presented by A.E.Hubbard With Contributions from R.L. Boivin, B.A. Carreras 1, S. Gangadhara, R. Granetz, M. Greenwald, J. Hughes, I. Hutchinson, J. Irby,

More information

Phase ramping and modulation of reflectometer signals

Phase ramping and modulation of reflectometer signals 4th Intl. Reflectometry Workshop - IRW4, Cadarache, March 22nd - 24th 1999 1 Phase ramping and modulation of reflectometer signals G.D.Conway, D.V.Bartlett, P.E.Stott JET Joint Undertaking, Abingdon, Oxon,

More information

Convective transport by intermittent blob-filaments: comparison of theory and experiment

Convective transport by intermittent blob-filaments: comparison of theory and experiment Convective transport by intermittent blob-filaments: comparison of theory and experiment D. A. D Ippolito 1, J. R. Myra 1 and S. J. Zweben 2 1Lodestar Research Corporation, Boulder, Colorado 2Princeton

More information

D. Smith, R. Fonck, G. McKee, D. Thompson, and I. Uzun-Kaymak

D. Smith, R. Fonck, G. McKee, D. Thompson, and I. Uzun-Kaymak College W&M Colorado Sch Mines Columbia U CompX General Atomics INL Johns Hopkins U LANL LLNL Lodestar MIT Nova Photonics New York U Old Dominion U ORNL PPPL PSI Princeton U Purdue U SNL Think Tank, Inc.

More information

Mean flows and blob velocities in scrape-off layer (SOLT) simulations of an L-mode discharge on Alcator C-Mod

Mean flows and blob velocities in scrape-off layer (SOLT) simulations of an L-mode discharge on Alcator C-Mod Mean flows and blob velocities in scrape-off layer (SOLT) simulations of an L-mode discharge on Alcator C-Mod D. A. Russell, J. R. Myra and D. A. D Ippolito Lodestar Research Corporation B. LaBombard,

More information

C-Mod Transport Program

C-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 information

Overview of the Geodesic Acoustic Mode (GAM) studies on the T-10 tokamak

Overview of the Geodesic Acoustic Mode (GAM) studies on the T-10 tokamak Overview of the Geodesic Acoustic Mode (GAM) studies on the T-10 tokamak A.V. Melnikov 1,2, L.G. Eliseev 1, L.I. Krupnik 3, J. Chercoles 4, A.A. Chmyga 3, G. N. Dezhko 3, M.A. Drabinskij 1, P.O. Khabanov

More information

Operational Phase Space of the Edge Plasma in Alcator C-Mod

Operational Phase Space of the Edge Plasma in Alcator C-Mod Operational Phase Space of the Edge Plasma in B. LaBombard, T. Biewer, M. Greenwald, J.W. Hughes B. Lipschultz, N. Smick, J.L. Terry, Team Contributed talk RO.00008 Presented at the 47th Annual Meeting

More information

EFFECT OF PLASMA FLOWS ON TURBULENT TRANSPORT AND MHD STABILITY*

EFFECT OF PLASMA FLOWS ON TURBULENT TRANSPORT AND MHD STABILITY* EFFECT OF PLASMA FLOWS ON TURBULENT TRANSPORT AND MHD STABILITY* by K.H. BURRELL Presented at the Transport Task Force Meeting Annapolis, Maryland April 3 6, 22 *Work supported by U.S. Department of Energy

More information

ArbiTER studies of filamentary structures in the SOL of spherical tokamaks

ArbiTER studies of filamentary structures in the SOL of spherical tokamaks ArbiTER studies of filamentary structures in the SOL of spherical tokamaks D. A. Baver, J. R. Myra, Research Corporation F. Scotti, Lawrence Livermore National Laboratory S. J. Zweben, Princeton Plasma

More information

Development of a New Gas Puff Imaging Diagnostic on the HL-2A Tokamak

Development of a New Gas Puff Imaging Diagnostic on the HL-2A Tokamak Development of a New Gas Puff Imaging Diagnostic on the HL-2A Tokamak B.Yuan a,b, M.Xu b,*, Y.Yu a,*, L.Zang b, R.Hong c, C.Chen b, Z.Wang b,l.nie b, R.Ke b, D.Guo b, Y.Wu a,b, T.Long b, S.Gong a,b, H.Liu

More information

Overview of Alcator C-Mod Research

Overview of Alcator C-Mod Research Overview of C-Mod Research Presented by E.S. Marmar On behalf of the C-Mod Team APS-DPP04 Paper JO3.001 Work Supported by USDoE Office of Fusion Energy Sciences SOL flows impose a toroidal rotation boundary

More information

L-to-H power threshold comparisons between NBI and RF heated plasmas in NSTX

L-to-H power threshold comparisons between NBI and RF heated plasmas in NSTX Research Supported by L-to-H power threshold comparisons between NBI and RF heated plasmas in NSTX T.M. Biewer 1, R. Maingi 1, H. Meyer 2, R.E. Bell 3, C. Bush 1, S. Kaye 3, S. Kubota 3, B. LeBlanc 3,

More information

Density Limit and Cross-Field Edge Transport Scaling in Alcator C-Mod

Density Limit and Cross-Field Edge Transport Scaling in Alcator C-Mod EX/D- Density Limit and Cross-Field Edge Transport Scaling in Alcator C-Mod B. LaBombard ), M. Greenwald ), R.L. Boivin ), B..A. Carreras 3), J.W. Hughes ), B. Lipschultz ), D. Mossessian ), C.S. Pitcher

More information

Pedestals and transitions in I-mode and comparison to H-mode

Pedestals and transitions in I-mode and comparison to H-mode Pedestals and transitions in I-mode and comparison to H-mode Amanda Hubbard, MIT Plasma Science and Fusion Center With thanks for input from J.W. Hughes, D. Brunner, M. Greenwald, B. LaBombard, A. Marinoni,

More information

Study of Enhanced D α H-modes Using the Alcator C-Mod Reflectometer

Study of Enhanced D α H-modes Using the Alcator C-Mod Reflectometer Study of Enhanced D α H-modes Using the Reflectometer Y. Lin 1, J.H. Irby, E.S. Marmar, R. Nazikian, M. Greenwald, A.E. Hubbard, J. Hughes, I.H. Hutchinson, B. LaBombard, A. Mazurenko, E. Nelson-Melby,

More information

TRANSPORT PROGRAM C-MOD 5 YEAR REVIEW MAY, 2003 PRESENTED BY MARTIN GREENWALD MIT PLASMA SCIENCE & FUSION CENTER

TRANSPORT 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 information

DIAGNOSTICS FOR ADVANCED TOKAMAK RESEARCH

DIAGNOSTICS 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 information

L-mode filament characteristics on MAST as a function of plasma current measured using visible imaging

L-mode filament characteristics on MAST as a function of plasma current measured using visible imaging 1 9/2/16 L-mode filament characteristics on MAST as a function of plasma current measured using visible imaging A. Kirk, A.J. Thornton, J.R. Harrison, F. Militello, N.R. Walkden and the MAST Team and the

More information

Alcator C-Mod. Particle Transport in the Alcator C-Mod Scrape-off Layer

Alcator C-Mod. Particle Transport in the Alcator C-Mod Scrape-off Layer Alcator C-Mod Particle Transport in the Alcator C-Mod Scrape-off Layer B. LaBombard, R.L. Boivin, B. Carreras, M. Greenwald, J. Hughes, B. Lipschultz, D. Mossessian, C.S. Pitcher, J.L. Terry, S.J. Zweben,

More information

EX/4-6Rb Electrostatic fluctuation and fluctuation-induced particle flux during formation of the edge transport barrier in the JFT-2M tokamak

EX/4-6Rb Electrostatic fluctuation and fluctuation-induced particle flux during formation of the edge transport barrier in the JFT-2M tokamak Electrostatic fluctuation and fluctuation-induced particle flux during formation of the edge transport barrier in the JFT-2M tokamak T. Ido 1), Y. Miura 2), K. Hoshino 2), Y. Hamada 1), Y. Nagashima 1),

More information

Characterization of Edge Stability and Ohmic H-mode in the PEGASUS Toroidal Experiment

Characterization of Edge Stability and Ohmic H-mode in the PEGASUS Toroidal Experiment Characterization of Edge Stability and Ohmic H-mode in the PEGASUS Toroidal Experiment M.W. Bongard, J.L. Barr, M.G. Burke, R.J. Fonck, E.T. Hinson, J.M. Perry, A.J. Redd, D.J. Schlossberg, K.E. Thome

More information

Dimensionless pedestal identity plasmas on Alcator C-Mod C

Dimensionless pedestal identity plasmas on Alcator C-Mod C Dimensionless pedestal identity plasmas on Alcator C-Mod C and JET G P Maddison 1, A E Hubbard 2, J W Hughes 2, I M Nunes 3, M N A Beurskens 1, S K Erents 1, Pasqualotto 4, E Giovannozzi 5, A Alfier 4,

More information

ELMs on C-Mod. J.W. Hughes for the Alcator C-Mod team. C-Mod/NSTX Pedestal Workshop Princeton, NJ September 7 8, 2010

ELMs on C-Mod. J.W. Hughes for the Alcator C-Mod team. C-Mod/NSTX Pedestal Workshop Princeton, NJ September 7 8, 2010 ELMs on C-Mod J.W. Hughes for the Alcator C-Mod team C-Mod/NSTX Pedestal Workshop Princeton, NJ September 7 8, 1 EDA H-mode is supplanted by small ELMs at higher beta 7 6 5 T e ped (ev) 4 3 Unstable Stable

More information

Impact of Localized ECRH on NBI and ICRH Driven Alfven Eigenmodes in the ASDEX Upgrade Tokamak

Impact of Localized ECRH on NBI and ICRH Driven Alfven Eigenmodes in the ASDEX Upgrade Tokamak Impact of Localized ECRH on NBI and ICRH Driven Alfven Eigenmodes in the ASDEX Upgrade Tokamak M. Garcia-Munoz M. A. Van Zeeland, S. Sharapov, Ph. Lauber, J. Ayllon, I. Classen, G. Conway, J. Ferreira,

More information

EXD/P3-13. Dependences of the divertor and midplane heat flux widths in NSTX

EXD/P3-13. Dependences of the divertor and midplane heat flux widths in NSTX 1 Dependences of the ertor and plane heat flux widths in NSTX T.K. Gray1,2), R. Maingi 2), A.G. McLean 2), V.A. Soukhanovskii 3) and J-W. Ahn 2) 1) Oak Ridge Institute for Science and Education (ORISE),

More information

Development and Validation of a Predictive Model for the Pedestal Height (EPED1)

Development and Validation of a Predictive Model for the Pedestal Height (EPED1) Development and Validation of a Predictive Model for the Pedestal Height (EPED1) P.B. Snyder 1 with R.J. Groebner 1, A.W. Leonard 1, T.H. Osborne 1, M. Beurskens 3, L.D. Horton 4, A.E. Hubbard 5, J.W.

More information

Plasma Fusion Center Massachusetts Institute of Technology Cambridge, MA Burrell, K.H. General Atomics PO Box San Diego, CA

Plasma Fusion Center Massachusetts Institute of Technology Cambridge, MA Burrell, K.H. General Atomics PO Box San Diego, CA PFC/JA-95-28 Edge Turbulence Measurements during the L- to H-Mode Transition by Phase Contrast Imaging on DIII-Dt Coda, S.; Porkolab, M.; Plasma Fusion Center Massachusetts Institute of Technology Cambridge,

More information

Alcator C-Mod. Double Transport Barrier Plasmas. in Alcator C-Mod. J.E. Rice for the C-Mod Group. MIT PSFC, Cambridge, MA 02139

Alcator C-Mod. Double Transport Barrier Plasmas. in Alcator C-Mod. J.E. Rice for the C-Mod Group. MIT PSFC, Cambridge, MA 02139 Alcator C-Mod Double Transport Barrier Plasmas in Alcator C-Mod J.E. Rice for the C-Mod Group MIT PSFC, Cambridge, MA 139 IAEA Lyon, Oct. 17, Outline Double Barrier Plasma Profiles and Modeling Conditions

More information

Long-Range Correlations and Edge Transport Bifurcation in Fusion Plasmas

Long-Range Correlations and Edge Transport Bifurcation in Fusion Plasmas EX-C/9-3 Long-Range Correlations and Edge Transport Bifurcation in Fusion Plasmas Y. Xu 1, N. Vianello 2, M. Spolaore 2, E. Martines 2, P. Manz 3, M. Ramisch 3, U. Stroth 3, C. Silva 4, M. A. Pedrosa 5,

More information

EXD/P3-23. Fluctuations, ELM Filaments and Turbulent Transport in the SOL at the Outer Midplane of ASDEX Upgrade

EXD/P3-23. Fluctuations, ELM Filaments and Turbulent Transport in the SOL at the Outer Midplane of ASDEX Upgrade Fluctuations, ELM Filaments and Turbulent Transport in the SOL at the Outer Midplane of ASDEX Upgrade H.W. Müller 1, J. Adamek 2, R. Cavazzana 3, G.D. Conway 1, J.P. Gunn 4, A. Herrmann 1, J. Horacek 2,

More information

Edge 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 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 information

Lower Hybrid Wave Induced Rotation on Alcator C-Mod* Ron Parker, Yuri Podpaly, John Rice, Andréa Schmidt

Lower Hybrid Wave Induced Rotation on Alcator C-Mod* Ron Parker, Yuri Podpaly, John Rice, Andréa Schmidt Lower Hybrid Wave Induced Rotation on Alcator C-Mod* Ron Parker, Yuri Podpaly, John Rice, Andréa Schmidt *Work supported by USDoE awards DE-FC-99ER551 and DE-AC-7CH373 Abstract Injection of RF power in

More information

SUMMARY OF EXPERIMENTAL CORE TURBULENCE CHARACTERISTICS IN OH AND ECRH T-10 TOKAMAK PLASMAS

SUMMARY OF EXPERIMENTAL CORE TURBULENCE CHARACTERISTICS IN OH AND ECRH T-10 TOKAMAK PLASMAS SUMMARY OF EXPERIMENTAL CORE TURBULENCE CHARACTERISTICS IN OH AND ECRH T-1 TOKAMAK PLASMAS V. Vershkov, L.G. Eliseev, S.A. Grashin. A.V. Melnikov, D.A. Shelukhin, S.V. Soldatov, A.O. Urazbaev and T-1 team

More information

Characterization of the Perpendicular Rotation Velocity of the Turbulence by Reflectometry in the Stellarator TJ-II

Characterization of the Perpendicular Rotation Velocity of the Turbulence by Reflectometry in the Stellarator TJ-II 1 EX/P5-31 Characterization of the Perpendicular Rotation Velocity of the Turbulence by Reflectometry in the Stellarator TJ-II T. Estrada 1), T. Happel 1), C. Hidalgo 1) 1) Laboratorio Nacional de Fusión.

More information

Lower Hybrid Current Drive Experiments on Alcator C-Mod: Comparison with Theory and Simulation

Lower Hybrid Current Drive Experiments on Alcator C-Mod: Comparison with Theory and Simulation Lower Hybrid Current Drive Experiments on Alcator C-Mod: Comparison with Theory and Simulation P.T. Bonoli, A. E. Hubbard, J. Ko, R. Parker, A.E. Schmidt, G. Wallace, J. C. Wright, and the Alcator C-Mod

More information

Propagation of Radio Frequency Waves Through Fluctuations in Plasmas

Propagation of Radio Frequency Waves Through Fluctuations in Plasmas PSFC/JA-15- Propagation of Radio Frequency Waves Through Fluctuations in Plasmas A. K. Ram K. Hizanidis a and S. Valvis a a National Technical University of Athens (part of HELLAS) School of Electrical

More information

Theory Work in Support of C-Mod

Theory 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 information

Investigations of pedestal turbulence and ELM bursts in NSTX H-mode plasmas

Investigations of pedestal turbulence and ELM bursts in NSTX H-mode plasmas Supported by Investigations of pedestal turbulence and ELM bursts in NSTX H-mode plasmas Coll of Wm & Mary Columbia U CompX General Atomics FIU INL Johns Hopkins U LANL LLNL Lodestar MIT Lehigh U Nova

More information

I-mode and H-mode plasmas at high magnetic field and pressure on Alcator C-Mod

I-mode and H-mode plasmas at high magnetic field and pressure on Alcator C-Mod I-mode and H-mode plasmas at high magnetic field and pressure on Alcator C-Mod A. E. Hubbard, J. W Hughes, S.-G. Baek, D. Brunner, I. Cziegler 1, E. Edlund, T. Golfinopoulos, M.J. Greenwald, J. Irby, B.

More information

Possible Pedestal Transport Theory Models And Modeling Tests

Possible Pedestal Transport Theory Models And Modeling Tests Possible Pedestal Transport Theory Models And Modeling Tests J.D. Callen, University of Wisconsin, Madison, WI 53706-1609 DIII-D Pedestal Transport Workshop, General Atomics, San Diego, CA, February 17,

More information

GA A27418 THE ROLE OF ZONAL FLOWS AND PREDATOR- PREY OSCILLATIONS IN THE FORMATION OF CORE AND EDGE TRANSPORT BARRIERS

GA A27418 THE ROLE OF ZONAL FLOWS AND PREDATOR- PREY OSCILLATIONS IN THE FORMATION OF CORE AND EDGE TRANSPORT BARRIERS GA A27418 THE ROLE OF ZONAL FLOWS AND PREDATOR- PREY OSCILLATIONS IN THE FORMATION OF CORE AND EDGE TRANSPORT BARRIERS by L. SCHMITZ, L. ZENG, T.L. RHODES, J.C. HILLESHEIM, W.A. PEEBLES, R.J. GROEBNER,

More information

Variation of Turbulence and Transport with the Te/Ti Ratio in H-Mode Plasmas

Variation of Turbulence and Transport with the Te/Ti Ratio in H-Mode Plasmas Variation of Turbulence and Transport with the Te/Ti Ratio in H-Mode Plasmas by G.R. McKee with C.H. Holland, C.C. Petty, H. Reimerdes,5, T.R. Rhodes6,L. Schmitz6, S. Smith, I.U. Uzun-Kaymak, G. Wang6,

More information

Observation of geodesic acoustic modes (GAMs) and their radial propagation at the edge of TEXTOR tokamak

Observation of geodesic acoustic modes (GAMs) and their radial propagation at the edge of TEXTOR tokamak Observation of geodesic acoustic modes (GAMs) and their radial propagation at the edge of TEXTOR tokamak Y. Xu 1, I. Shesterikov 1, M. Van Schoor 1, M. Vergote 1, R. R. Weynants 1, A. Krämer-Flecken 2,

More information

L-H transitions driven by ion heating in scrape-off layer turbulence (SOLT) model simulations

L-H transitions driven by ion heating in scrape-off layer turbulence (SOLT) model simulations L-H transitions driven by ion heating in scrape-off layer turbulence (SOLT) model simulations D.A. Russell, D.A. D Ippolito and J.R. Myra Research Corporation, Boulder, CO, USA Presented at the 015 Joint

More information

Particle transport results from collisionality scans and perturbative experiments on DIII-D

Particle transport results from collisionality scans and perturbative experiments on DIII-D 1 EX/P3-26 Particle transport results from collisionality scans and perturbative experiments on DIII-D E.J. Doyle 1), L. Zeng 1), G.M. Staebler 2), T.E. Evans 2), T.C. Luce 2), G.R. McKee 3), S. Mordijck

More information

1) H-mode in Helical Devices. 2) Construction status and scientific objectives of the Wendelstein 7-X stellarator

1) H-mode in Helical Devices. 2) Construction status and scientific objectives of the Wendelstein 7-X stellarator Max-Planck-Institut für Plasmaphysik 1) H-mode in Helical Devices M. Hirsch 1, T. Akiyama 2, T.Estrada 3, T. Mizuuchi 4, K. Toi 2, C. Hidalgo 3 1 Max-Planck-Institut für Plasmaphysik, EURATOM-Ass., D-17489

More information

Beam Driven Alfvén Eigenmodes and Fast Ion Transport in the DIII-D and ASDEX Upgrade (AUG) Tokamaks

Beam Driven Alfvén Eigenmodes and Fast Ion Transport in the DIII-D and ASDEX Upgrade (AUG) Tokamaks Beam Driven Alfvén Eigenmodes and Fast Ion Transport in the DIII-D and ASDEX Upgrade (AUG) Tokamaks by M.A. Van Zeeland 1 M. García-Muñoz 2, W.W. Heidbrink 3, I. Classen 4, R.K. Fisher 1, B. Geiger 2,

More information

Experimental Achievements on Plasma Confinement and Turbulence

Experimental Achievements on Plasma Confinement and Turbulence Experimental Achievements on Plasma Confinement and Turbulence Akihide Fujisawa National Institute for Fusion Science since ~9 Zonal-flow Helical Plasma ITER- Summer School 28 in Fukuoka Japan Introduction

More information

Direct drive by cyclotron heating can explain spontaneous rotation in tokamaks

Direct drive by cyclotron heating can explain spontaneous rotation in tokamaks Direct drive by cyclotron heating can explain spontaneous rotation in tokamaks J. W. Van Dam and L.-J. Zheng Institute for Fusion Studies University of Texas at Austin 12th US-EU Transport Task Force Annual

More information

1. INTRODUCTION. PACS numbers: Ra, g, Xz, Kt, Mw, Cb

1. INTRODUCTION. PACS numbers: Ra, g, Xz, Kt, Mw, Cb Investigating flow patterns and related dynamics in multi-instability turbulent plasmas using a three-point cross-phase time delay estimation velocimetry scheme C. Brandt 1,, S. C. Thakur 1,3, G. R. Tynan

More information

On the physics of shear flows in 3D geometry

On the physics of shear flows in 3D geometry On the physics of shear flows in 3D geometry C. Hidalgo and M.A. Pedrosa Laboratorio Nacional de Fusión, EURATOM-CIEMAT, Madrid, Spain Recent experiments have shown the importance of multi-scale (long-range)

More information

Evidence for Electromagnetic Fluid Drift Turbulence Controlling the Edge Plasma State in Alcator C-Mod

Evidence for Electromagnetic Fluid Drift Turbulence Controlling the Edge Plasma State in Alcator C-Mod Evidence for Electromagnetic Fluid Drift Turbulence Controlling the Edge Plasma State in B. LaBombard, J.W. Hughes, D. Mossessian, M. Greenwald, J.L. Terry, Team Contributed talk CO.00 Presented at the

More information

OVERVIEW 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 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 information

Characteristics of the H-mode H and Extrapolation to ITER

Characteristics of the H-mode H and Extrapolation to ITER Characteristics of the H-mode H Pedestal and Extrapolation to ITER The H-mode Pedestal Study Group of the International Tokamak Physics Activity presented by T.Osborne 19th IAEA Fusion Energy Conference

More information

Turbulence and geodesic acoustic mode behavioural studies in ASDEX Upgrade using Doppler Reflectometry

Turbulence and geodesic acoustic mode behavioural studies in ASDEX Upgrade using Doppler Reflectometry 1 IAEA-CN-165 / EX / P5-38 Turbulence and geodesic acoustic mode behavioural studies in ASDEX Upgrade using Doppler Reflectometry G.D.Conway 1, C.Tröster 1, J.Schirmer 1, W.Suttrop 1, C.Lechte 2, E.Holzhauer

More information

Effect of RMPs on the edge turbulence in ohmic and L-mode plasmas

Effect of RMPs on the edge turbulence in ohmic and L-mode plasmas Max-Planck-Institut für Plasmaphysik Effect of RMPs on the edge turbulence in ohmic and L-mode plasmas 1, Ph. Ghendrih2, A. Kirk3, O. Schmitz4, W. Suttrop1, P. Tamain3, Y. Xu5, and the ASDEX Upgrade Team1

More information

ELMs and Constraints on the H-Mode Pedestal:

ELMs and Constraints on the H-Mode Pedestal: ELMs and Constraints on the H-Mode Pedestal: A Model Based on Peeling-Ballooning Modes P.B. Snyder, 1 H.R. Wilson, 2 J.R. Ferron, 1 L.L. Lao, 1 A.W. Leonard, 1 D. Mossessian, 3 M. Murakami, 4 T.H. Osborne,

More information

Flow, turbulence and transport in laboratory plasmas (at least in LAPD and DIII-D)

Flow, turbulence and transport in laboratory plasmas (at least in LAPD and DIII-D) Flow, turbulence and transport in laboratory plasmas (at least in LAPD and DIII-D) T.A. Carter, D. Schaffner, B. Friedman, J. Hillesheim, W.A. Peebles, G. Rossi, M.V. Umansky 2, D. Guice, S. Vincena, J.E.

More information

ABSTRACT, POSTER LP1 12 THURSDAY 11/7/2001, APS DPP CONFERENCE, LONG BEACH. Recent Results from the Quiescent Double Barrier Regime on DIII-D

ABSTRACT, POSTER LP1 12 THURSDAY 11/7/2001, APS DPP CONFERENCE, LONG BEACH. Recent Results from the Quiescent Double Barrier Regime on DIII-D ABSTRACT, POSTER LP1 1 THURSDAY 11/7/1, APS DPP CONFERENCE, LONG BEACH Recent Results from the Quiescent Double Barrier Regime on DIII-D E.J. Doyle, K.H. Burrell, T. Casper, J.C. DeBoo, A. Garofalo, P.

More information

Issues of Perpendicular Conductivity and Electric Fields in Fusion Devices

Issues of Perpendicular Conductivity and Electric Fields in Fusion Devices Issues of Perpendicular Conductivity and Electric Fields in Fusion Devices Michael Tendler, Alfven Laboratory, Royal Institute of Technology, Stockholm, Sweden Plasma Turbulence Turbulence can be regarded

More information

Particle and Energy Transport in the SOL of DIII-D and NSTX

Particle and Energy Transport in the SOL of DIII-D and NSTX 1 EX/P4-2 Particle and Energy Transport in the SOL of DIII-D and NSTX J.A. Boedo 1), R.J. Maqueda 2), D.L. Rudakov 1), G.R. McKee 3), H. Kugel 4), R. Maingi 5), N. Crocker 6), R.A. Moyer 1), V.A. Soukhanovskii

More information

A 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 * 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 information

Investigation of causes for the discrepancy between the measured and modeled helium emissions using a gas puff imaging diagnostic

Investigation of causes for the discrepancy between the measured and modeled helium emissions using a gas puff imaging diagnostic Investigation of causes for the discrepancy between the measured and modeled helium emissions using a gas puff imaging diagnostic S. Baek, J. Terry, D. P. Stotler*, D. Brunner, B. LaBombard MIT Plasma

More information

Characteristics of Energetic-Ion-Driven Geodesic Acoustic Modes in the Large Helical Device(LHD)

Characteristics 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 information

Electron temperature barriers in the RFX-mod experiment

Electron temperature barriers in the RFX-mod experiment Electron temperature barriers in the RFX-mod experiment A. Scaggion Consorzio RFX, Padova, Italy Tuesday 5 th October 2010 ADVANCED PHYSICS LESSONS 27/09/2010 07/10/2010 IPP GARCHING JOINT EUROPEAN RESEARCH

More information

Dependences of Critical Rotational Shear in DIII-D QH-mode Discharges

Dependences of Critical Rotational Shear in DIII-D QH-mode Discharges Dependences of Critical Rotational Shear in DIII-D QH-mode Discharges by T.M. Wilks 1 with K.H. Burrell 2, Xi. Chen 2, A. Garofalo 2, R.J. Groebner 2, P. Diamond 3, Z. Guo 3, and J.W. Hughes 1 1 MIT 2

More information

Studies of Lower Hybrid Range of Frequencies Actuators in the ARC Device

Studies of Lower Hybrid Range of Frequencies Actuators in the ARC Device Studies of Lower Hybrid Range of Frequencies Actuators in the ARC Device P. T. Bonoli, Y. Lin. S. Shiraiwa, G. M. Wallace, J. C. Wright, and S. J. Wukitch MIT PSFC, Cambridge, MA 02139 59th Annual Meeting

More information

NSTX. Electron gyro-scale fluctuations in NSTX plasmas. David Smith, PPPL. Supported by

NSTX. Electron gyro-scale fluctuations in NSTX plasmas. David Smith, PPPL. Supported by NSTX Supported by Electron gyro-scale fluctuations in NSTX plasmas College W&M Colorado Sch Mines Columbia U Comp-X General Atomics INEL Johns Hopkins U LANL LLNL Lodestar MIT Nova Photonics New York U

More information

Characterization of neo-classical tearing modes in high-performance I- mode plasmas with ICRF mode conversion flow drive on Alcator C-Mod

Characterization of neo-classical tearing modes in high-performance I- mode plasmas with ICRF mode conversion flow drive on Alcator C-Mod 1 EX/P4-22 Characterization of neo-classical tearing modes in high-performance I- mode plasmas with ICRF mode conversion flow drive on Alcator C-Mod Y. Lin, R.S. Granetz, A.E. Hubbard, M.L. Reinke, J.E.

More information

Initial Investigations of H-mode Edge Dynamics in the PEGASUS Toroidal Experiment

Initial Investigations of H-mode Edge Dynamics in the PEGASUS Toroidal Experiment Initial Investigations of H-mode Edge Dynamics in the PEGASUS Toroidal Experiment M.W. Bongard, R.J. Fonck, K.E. Thome, D.S. Thompson 55 th Annual Meeting of the APS Division of Plasma Physics University

More information

PSI meeting, Aachen Germany, May 2012

PSI meeting, Aachen Germany, May 2012 Constraining the divertor heat width in ITER D.G. Whyte 1, B. LaBombard 1, J.W. Hughes 1, B. Lipschultz 1, J. Terry 1, D. Brunner 1, P.C. Stangeby 2, D. Elder 2, A.W. Leonard 3, J. Watkins 4 1 MIT Plasma

More information

Active and Fast Particle Driven Alfvén Eigenmodes in Alcator C-Mod

Active and Fast Particle Driven Alfvén Eigenmodes in Alcator C-Mod Active and Fast Particle Driven Alfvén Eigenmodes in Alcator C-Mod JUST DID IT. J A Snipes, N Basse, C Boswell, E Edlund, A Fasoli #, N N Gorelenkov, R S Granetz, L Lin, Y Lin, R Parker, M Porkolab, J

More information

- Effect of Stochastic Field and Resonant Magnetic Perturbation on Global MHD Fluctuation -

- Effect of Stochastic Field and Resonant Magnetic Perturbation on Global MHD Fluctuation - 15TH WORKSHOP ON MHD STABILITY CONTROL: "US-Japan Workshop on 3D Magnetic Field Effects in MHD Control" U. Wisconsin, Madison, Nov 15-17, 17, 2010 LHD experiments relevant to Tokamak MHD control - Effect

More information

The current status of the Lithium beam diagnostic at ASDEX Upgrade

The current status of the Lithium beam diagnostic at ASDEX Upgrade The current status of the Lithium beam diagnostic at ASDEX Upgrade Elisabeth Wolfrum Josef Schweinzer Matthias Reich Rainer Fischer Max Planck Institut für Plasmaphysik Garching, Germany Outline Experimental

More information

Evidence for electromagnetic fluid drift turbulence controlling the edge plasma state in the Alcator C-Mod tokamak

Evidence for electromagnetic fluid drift turbulence controlling the edge plasma state in the Alcator C-Mod tokamak PSFC/JA-05-4 Evidence for electromagnetic fluid drift turbulence controlling the edge plasma state in the Alcator C-Mod tokamak B. LaBombard, J.W. Hughes, D. Mossessian, M. Greenwald, B. Lipschultz, J.L.

More information

Improved Plasma Confinement by Ion Bernstein Waves (IBWs) Interacting with Ions in JET (Joint European Torus)

Improved Plasma Confinement by Ion Bernstein Waves (IBWs) Interacting with Ions in JET (Joint European Torus) Improved Plasma Confinement by Ion Bernstein Waves (IBWs) Interacting with Ions in JET (Joint European Torus) PD/P-01 C. Castaldo 1), R. Cesario 1), Y, Andrew 2), A. Cardinali 1), V. Kiptly 2), M. Mantsinen

More information

Enhanced Energy Confinement Discharges with L-mode-like Edge Particle Transport*

Enhanced Energy Confinement Discharges with L-mode-like Edge Particle Transport* Enhanced Energy Confinement Discharges with L-mode-like Edge Particle Transport* E. Marmar, B. Lipschultz, A. Dominguez, M. Greenwald, N. Howard, A. Hubbard, J. Hughes, B. LaBombard, R. McDermott, M. Reinke,

More information

David R. Smith UW-Madison

David R. Smith UW-Madison Supported by College W&M Colorado Sch Mines Columbia U Comp-X General Atomics INEL Johns Hopkins U LANL LLNL Lodestar MIT Nova Photonics New York U Old Dominion U ORNL PPPL PSI Princeton U Purdue U SNL

More information