Stereoscopic Pellet Imaging

Slides:



Advertisements
Similar presentations
Statistical Properties of Broadband Magnetic Turbulence in the Reversed Field Pinch John Sarff D. Craig, L. Frassinetti 1, L. Marrelli 1, P. Martin 1,
Advertisements

NONLINEAR COMPUTATION OF LABORATORY DYNAMOS DALTON D. SCHNACK Center for Energy and Space Science Science Applications International Corp. San Diego, CA.
Development of experimental devices to study first wall conditioning and transport phenomena in RFX-mod experiment Stefano Munaretto Università degli studi.
Particle’s Dynamics in Dusty Plasma with Gradients of Dust Charges
9th TTF Spain September 11, 2002 B. J. Peterson, NIFS, Japan page 1 Radiative Collapse and Density Limit in the Large Helical Device.
Particle acceleration in a turbulent electric field produced by 3D reconnection Marco Onofri University of Thessaloniki.
Institute of Interfacial Process Engineering and Plasma Technology Gas-puff imaging of blob filaments at ASDEX Upgrade TTF Workshop.
Fine-scale 3-D Dynamics of Critical Plasma Regions: Necessity of Multipoint Measurements R. Lundin 1, I. Sandahl 1, M. Yamauchi 1, U. Brändström 1, and.
A. Kirk, 20th IAEA Fusion Energy Conference, Vilamoura, Portugal, 2004 The structure of ELMS and the distribution of transient power loads in MAST Presented.
Ion Pickup One of the fundamental processes in space plasma physics.
William Daughton Plasma Physics Group, X-1 Los Alamos National Laboratory Presented at: Second Workshop on Thin Current Sheets University of Maryland April.
INTRODUCTION OF WAVE-PARTICLE RESONANCE IN TOKAMAKS J.Q. Dong Southwestern Institute of Physics Chengdu, China International School on Plasma Turbulence.
Modeling Generation and Nonlinear Evolution of Plasma Turbulence for Radiation Belt Remediation Center for Space Science & Engineering Research Virginia.
Nonlinear Evolution of Whistler Turbulence W.A. Scales, J.J. Wang, and O. Chang Center of Space Science and Engineering Research Virginia Tech L. Rudakov,
Plasma Dynamics Lab HIBP Abstract Measurements of the radial equilibrium potential profiles have been successfully obtained with a Heavy Ion Beam Probe.
Results from Visible Light Imaging of Alfvén Fluctuations in the H-1NF Heliac J. Read, J. Howard, B. Blackwell, David Oliver, & David Pretty Acknowledgements:
Some results / ideas on the effect of flows D. Strintzi, C. Angioni, A. Bottino, A.G. Peeters.
Hybrid simulations of parallel and oblique electromagnetic alpha/proton instabilities in the solar wind Q. M. Lu School of Earth and Space Science, Univ.
Plasma Dynamics Lab HIBP Abstract Measurements of the radial equilibrium potential profiles have been successfully obtained with a Heavy Ion Beam Probe.
N.Vianello 09 October t h IEA/RFP Workshop Current filaments and electrostatic structures measured in the edge region of the RFX-mod experiment.
Plasma Kinetics around a Dust Grain in an Ion Flow N F Cramer and S V Vladimirov, School of Physics, University of Sydney, S A Maiorov, General Physics.
6 th Japan-Korea Workshop on Theory and Simulation of Magnetic Fusion Plasmas Hyunsun Han, G. Park, Sumin Yi, and J.Y. Kim 3D MHD SIMULATIONS.
Kinetic Effects on the Linear and Nonlinear Stability Properties of Field- Reversed Configurations E. V. Belova PPPL 2003 APS DPP Meeting, October 2003.
Hybrid Simulations of Energetic Particle-driven Instabilities in Toroidal Plasmas Guo-Yong Fu In collaboration with J. Breslau, J. Chen, E. Fredrickson,
Particle Distribution Modification by TAE mode and Resonant Particle Orbits POSTECH 1, NFRI 1,2 M.H.Woo 1, C.M.Ryu 1, T.N.Rhee 1,,2.
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.
ASIPP On the observation of small scale turbulence on HT-7 tokamak* Tao Zhang**, Yadong Li, Shiyao Lin, Xiang Gao, Junyu Zhao, Qiang Xu Institute of Plasma.
Flow and Shear behavior in the Edge and Scrape- off Layer in NSTX L-Mode Plasmas Y. Sechrest and T. Munsat University of Colorado at Boulder S. J. Zweben.
Stability Properties of Field-Reversed Configurations (FRC) E. V. Belova PPPL 2003 International Sherwood Fusion Theory Conference Corpus Christi, TX,
1 Results and analysis of Gas Puff Imaging experiments in NSTX: turbulence, L-H transitions, ELMs and other phenomena R.J. Maqueda Nova Photonics S.J.
Nonlinear interactions between micro-turbulence and macro-scale MHD A. Ishizawa, N. Nakajima, M. Okamoto, J. Ramos* National Institute for Fusion Science.
Association EURATOM-CEA Electromagnetic Self-Organization and Turbulent Transport in Tokamaks G. Fuhr, S. Benkadda, P. Beyer France Japan Magnetic Fusion.
NSTX APS DPP 2008 – RWM Stabilization in NSTX (Berkery)November 19, Resistive Wall Mode stabilization in NSTX may be explained by kinetic theory.
ASIPP 1 EAST 上充气成像诊断研制及边界湍流 实验研究 邵林明 导师:徐国盛
Kansas Annual NSF EPSCoR Statewide Conference Wichita, KSJanuary 12-13, 2012 Simulation of pellet ablation in DIII-D Tianshi Lu Patrick Rinker Department.
Kinetic MHD Simulation in Tokamaks H. Naitou, J.-N. Leboeuf †, H. Nagahara, T. Kobayashi, M. Yagi ‡, T. Matsumoto*, S. Tokuda* Joint Meeting of US-Japan.
Objectives Much better spatial resolution Velocity space discrimination W. Heidbrink, M. Van Zeeland, J. Yu FIDA Imaging Proposal.
Radiation spectra from relativistic electrons moving in turbulent magnetic fields Yuto Teraki & Fumio Takahara Theoretical Astrophysics Group Osaka Univ.,
Simulations of NBI-driven Global Alfven Eigenmodes in NSTX E. V. Belova, N. N. Gorelenkov, C. Z. Cheng (PPPL) NSTX Results Forum, PPPL July 2006 Motivation:
Association Euratom-CEA TORE SUPRA EAST, China 07/01/2010Xiaolan Zou1 Xiaolan ZOU CEA, IRFM, F Saint-Paul-Lez-Durance, France Heat and Particle Transport.
Numerical Study on Ideal MHD Stability and RWM in Tokamaks Speaker: Yue Liu Dalian University of Technology, China Co-Authors: Li Li, Xinyang Xu, Chao.
1 Observations of Linear and Nonlinear Dust Acoustic Waves* Bob Merlino, Jon Heinrich Su Hyun Kim and John Meyer Department of Physics and Astronomy The.
Nonlinear Simulations of Energetic Particle-driven Modes in Tokamaks Guoyong Fu Princeton Plasma Physics Laboratory Princeton, NJ, USA In collaboration.
Simulation of Turbulence in FTU M. Romanelli, M De Benedetti, A Thyagaraja* *UKAEA, Culham Sciance Centre, UK Associazione.
Interaction between vortex flow and microturbulence Zheng-Xiong Wang (王正汹) Dalian University of Technology, Dalian, China West Lake International Symposium.
Nonlinear plasma-wave interactions in ion cyclotron range of frequency N Xiang, C. Y Gan, J. L. Chen, D. Zhou Institute of plasma phsycis, CAS, Hefei J.
Supported by Experimental studies of ion-scale fluctuations via microwave imaging reflectometry in KSTAR 5 th EAST-Asia School and Workshop (EASW) on Laboratory,
Energetic ion excited long-lasting “sword” modes in tokamak plasmas with low magnetic shear Speaker:RuiBin Zhang Advisor:Xiaogang Wang School of Physics,
T. Biewer, Sep. 20 th, 2004 NSTX Results Review of 11 Edge Ion Heating by Launched HHFW in NSTX T.M. Biewer, R.E. Bell, S. Diem, P.M. Ryan, J.R.
An overview of turbulent transport in tokamaks
25th IAEA FUSION ENERGY CONFERENCE EX/11-3
33 (6 outlines) -> 27.
Date of download: 10/31/2017 Copyright © ASME. All rights reserved.
DIII-D Frontiers Science Proposal Template
Substorm current wedge, Alfven waves, ion injections, Pi2 pulsations, and ion outflows: A THEMIS look The THEMIS team.
Sunny Ri Li, Nasser Ashgriz
Substorm current wedge, Alfven waves, ion injections, Pi2 pulsations, and ion outflows: A THEMIS look The THEMIS team.
Motion of Charged Particles
Influence of energetic ions on neoclassical tearing modes
Visible Doppler Spectrometer for Edge Toroidal Rotation
Stereoscopic Pellet Imaging
Evaluation of the main ion flow and temperature using the GPI system
DOE Plasma Science Center Control of Plasma Kinetics
Parallel Structure of Edge Turbulence
Momentum Transport and Rotation Studies
2-4 Acceleration Acceleration is the rate of change of velocity.
Stabilization of m/n=1/1 fishbone by ECRH
XGC simulation of CMOD edge plasmas
Reflectometry measurements of turbulence in Alcator C-Mod plasmas
Electron Acoustic Waves (EAW) EAW’s are novel kinetic waves that exist only because nonlinear trapping turns off Landau damping. We recently provided.
Presentation transcript:

Stereoscopic Pellet Imaging Motivation Pellet injection during previous campaigns has revealed the presence of striated structure during the evolution of the pellet ablation. Furthermore, this striated structure has qualitatively different behavior during L-Mode and H-Mode operation. L-Mode shots have striations that move in both the positive and negative ion diamagnetic velocity. Striations in H-Mode move purely in the negative ion diamagnetic drift direction. Shot 1020827021

Stereoscopic Pellet Imaging Mid Plane 42.4 inches 9.56” Camera Views Pellet Trajectory Idea Using the stereoscopic imaging system recently developed for C-Mod, we would like to image a large number of pellet shots during different modes of plasma operation to gather three dimensional data on the ablation process and evolution of the striations, and determine what effect the background plasma conditions have on the striations. This data will be compared with poloidal flows determined by gyro kinetic simulations to determine if any correlation exists. 9.56”

Stereoscopic Pellet Imaging Expected Results Observation of growth of Raleigh-Taylor instability that drives striation formation Stereoscopic imaging should be able to discern whether the cloud is rotating prior to the striation formation, and determine the rotation rate. Parks Predicts that the rotation rate, and instability frequency should go like: Determine whether striation formation has a temporal or spatial scaling The Parks instability theory predicts that the frequency of striation emission should be independent of the position of the pellet. If the striation motion is a function of the local poloidal flows in the plasma then distribution of the striation velocities will be correlated with the structure of the poloidal flows. Observe scaling of poloidal flows. Theory and Gyro-kinetic simulations indicate that the magnitude of poloidal flows should go like