Toroidal rotation in ECRH L-mode, I-phase and H-mode on HL-2A tokamak A.P. Sun, J.Q. Dong, X.Y. Han, C.H. Liu, J.Y. Cao, M. Huang, Y.G. Li, X. L. Huang.

Slides:



Advertisements
Similar presentations
Ion Heating and Velocity Fluctuation Measurements in MST Sanjay Gangadhara, Darren Craig, David Ennis, Gennady Fiskel and the MST team University of Wisconsin-Madison.
Advertisements

Current status of H-mode/pedestal related experiments in JT-60U 14th meeting of the ITPA-TG on Pedestal&Edge Physics Group, General Atomics, April 29-May.
PPRC PPRC IR-T1 Tokamak Experimental Programme, Plans and Recent Results IR-T1 Tokamak Experimental Programme, Plans and Recent Results Presented By P.
ASIPP Characteristics of edge localized modes in the superconducting tokamak EAST M. Jiang Institute of Plasma Physics Chinese Academy of Sciences The.
Institute of Interfacial Process Engineering and Plasma Technology Gas-puff imaging of blob filaments at ASDEX Upgrade TTF Workshop.
A. Kirk, 21 st IAEA Fusion Energy Conference, Chengdu, China, October 2006 Evolution of the pedestal on MAST and the implications for ELM power loadings.
1 J-W. Ahn a H.S. Han b, H.S. Kim c, J.S. Ko b, J.H. Lee d, J.G. Bak b, C.S. Chang e, D.L. Hillis a, Y.M. Jeon b, J.G. Kwak b, J.H. Lee b, Y. S. Na c,
INTRODUCTION OF WAVE-PARTICLE RESONANCE IN TOKAMAKS J.Q. Dong Southwestern Institute of Physics Chengdu, China International School on Plasma Turbulence.
Measurement of magnetic island width by using multi-channel ECE radiometer on HT-7 tokamak Han Xiang( 韩翔 ), Ling Bili( 凌必利 ), Gao Xiang( 高翔 ), Liu Yong(
New Experimental Results Obtained using Microwave Reflectometry in HL-2A Tokamak W.W. Xiao1), X.T. Ding1), X.L. Zou2), Z.T. Liu1), Y.D. Gao1), J.Q. Dong1),
Temporal evolution of plasma rotation measurement in tokamaks using an optical monochromator and two photomultipliers as detector Severo J. H. F. .
Energy loss for grassy ELMs and effects of plasma rotation on the ELM characteristics in JT-60U N. Oyama 1), Y. Sakamoto 1), M. Takechi 1), A. Isayama.
49th Annual Meeting of the Division of Plasma Physics, November , 2007, Orlando, Florida Ion Temperature Measurements and Impurity Radiation in.
D. Borba 1 21 st IAEA Fusion Energy Conference, Chengdu China 21 st October 2006 Excitation of Alfvén eigenmodes with sub-Alfvénic neutral beam ions in.
A. HerrmannITPA - Toronto /19 Filaments in the SOL and their impact to the first wall EURATOM - IPP Association, Garching, Germany A. Herrmann,
Recent Results from the STOR-M Tokamak A.Hirose, M. Dreval, S. Elgriw, O. Mitarai(1), A. Pant, M. Peng(2), D. Rohraff, A.K. Singh(3), D. Trembach, C. Xiao.
Nils P. Basse Plasma Science and Fusion Center Massachusetts Institute of Technology Cambridge, MA USA ABB seminar November 7th, 2005 Measurements.
H. Urano, H. Takenaga, T. Fujita, Y. Kamada, K. Kamiya, Y. Koide, N. Oyama, M. Yoshida and the JT-60 Team Japan Atomic Energy Agency JT-60U Tokamak: p.
10th ITPA TP Meeting - 24 April A. Scarabosio 1 Spontaneous stationary toroidal rotation in the TCV tokamak A. Scarabosio, A. Bortolon, B. P. Duval,
Study of transport simulation on RF heated and current driven EAST plasma Siye Ding Under instruction of Prof. Baonian Wan 12/09/2009.
Profile Measurement of HSX Plasma Using Thomson Scattering K. Zhai, F.S.B. Anderson, J. Canik, K. Likin, K. J. Willis, D.T. Anderson, HSX Plasma Laboratory,
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,
L. Chen US TTF meeting, 2014 April 22-25, San Antonio, Texas 1 Study on Power Threshold of the L-I-H Transition on the EAST Superconducting Tokamak L.
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.
Review of Collaboration Activities J.Q. Dong* H.D. He, Y. Shen, and A.P. Sun Southwestern Institute of Physics, China *Institute for Fusion Theory and.
TITLE: Scaling of the far SOL turbulence as a function of (1), the average density keeping other plasma parameters constant. (3), the plasma current keeping.
12/03/2013, Praga 1 Plasma MHD Activity Observations via Magnetics Diagnostics: Magnetic island Analysis Magnetic island Analysis Frederik Ostyn (UGent)
High  p experiments in JET and access to Type II/grassy ELMs G Saibene and JET TF S1 and TF S2 contributors Special thanks to to Drs Y Kamada and N Oyama.
1 Plasma Rotation and Momentum Confinement – DB ITPA - 1 October 2007 by Peter de Vries Plasma Rotation and Momentum Confinement Studies at JET P.C. de.
EAST Data processing of divertor probes on EAST Jun Wang, Jiafeng Chang, Guosheng Xu, Wei Zhang, Tingfeng Ming, Siye Ding Institute of Plasma Physics,
NSTX Boundary Density Fluctuation Measurement by FIReTIP System with USN/LSN Configurations K.C. Lee, C.W. Domier, M. Johnson, N.C. Luhmann, Jr. University.
Recent Results of KSTAR
Upgrade Plan of FIReTIP System and Toroidal Magnetic Field Measured by Polarimetry on NSTX* K.C. Lee, C.W. Domier, M. Johnson, H. Chen, N.C. Luhmann, Jr.
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.
ASIPP Long pulse and high power LHCD plasmas on HT-7 Xu Qiang.
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.
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.
U NIVERSITY OF S CIENCE AND T ECHNOLOGY OF C HINA CAS K EY L ABORATORY OF B ASIC P LASMA P HYSICS Recent experimental results of zonal flows in edge tokamak.
Session I-B – Overview Talks Lithium in Magnetic Confinement Experiments S. MirnovLi collection experiments on T-11M and T-10 in framework of Li closed.
Radial Electric Field Formation by Charge Exchange Reaction at Boundary of Fusion Device* K.C. Lee U.C. Davis *submitted to Physics of Plasmas.
CCFE is the fusion research arm of the United Kingdom Atomic Energy Authority ITB formation and evolution with co- and counter NBI A. R. Field, R. J. Akers,
HL-2A Heating & Current Driving by LHW and ECW study on HL-2A Bai Xingyu, HL-2A heating team.
N. Nishino, T. Mizuuchi a, S.Kobayashi a, S.Yamamoto a, H.Okada a, K.Nagasaki a, T.Minami a, F.Sano a ISHW /10/13 PPPL Peripheral plasma measurement.
1 L.W. Yan, Overview on HL-2A, 23rd IAEA FEC, Oct. 2010, Daejeon, Republic of Korea HL-2A 2 nd Asia-Pacific Transport Working Group Meeting ELM mitigation.
Improved performance in long-pulse ELMy H-mode plasmas with internal transport barrier in JT-60U N. Oyama, A. Isayama, T. Suzuki, Y. Koide, H. Takenaga,
1 LHCD Properties with a New Lower Hybrid Wave Antenna on HT-7 Tokamak Wei Wei,Guangli Kuang,Bojiang Ding,Weici Shen and HT-7 Team Institute of Plasma.
Confinement & Transport Plan Classical theory of confinement and transport. o Diffusion equation Particle diffusion in a magnetic field.
Changes in Edge Turbulence with  * and Toroidal Rotation Input in NSTX M. Gilmore, S. Kubota, W.A. Peebles, and X.V. Nguyen Electrical Engineering Dept.,
20th IAEA Fusion Energy Conference, 2004 Naka Fusion Research Establishment, Japan Atomic Energy Research Institute Stationary high confinement plasmas.
LI et al. 1 G.Q. Li 1, X.Z. Gong 1, A.M. Garofalo 2, L.L. Lao 2, O. Meneghini 2, P.B. Snyder 2, Q.L. Ren 1, S.Y. Ding 1, W.F. Guo 1, J.P. Qian 1, B.N.
Plasma MHD Activity Observations via Magnetic Diagnostics Magnetic islands, statistical methods, magnetic diagnostics, tokamak operation.
Page 1 Alberto Loarte- NSTX Research Forum st - 3 rd December 2009  ELM control by RMP is foreseen in ITER to suppress or reduce size of ELM energy.
1) For equivalent ECRH power, off-axis heating results in lower stored energy and lower core temperature 2) Plasma flow is significantly reduced with off-axis.
1 NSTX EXPERIMENTAL PROPOSAL - OP-XP-712 Title: HHFW Power Balance Optimization at High B Field J. Hosea, R. Bell, S. Bernabei, L. Delgado-Aparicio, S.
Scaling experiments of perturbative impurity transport in NSTX D. Stutman, M. Finkenthal Johns Hopkins University J. Menard, E. Synakowski, B. Leblanc,R.
1 ASIPP Sawtooth Stabilization by Barely Trapped Energetic Electrons Produced by ECRH Zhou Deng, Wang Shaojie, Zhang Cheng Institute of Plasma Physics,
T. Biewer, Sep. 21 st, 2004 NSTX Results Review of 11 Dependence of Edge Flow on Magnetic Configuration in NSTX T.M. Biewer, R.E. Bell, D. Gates,
Plan V. Rozhansky, E. Kaveeva St.Petersburg State Polytechnical University, , Polytechnicheskaya 29, St.Petersburg, Russia Poloidal and Toroidal.
HT-7 ASIPP Investigation on Z eff and impurities behavior with molybdenum limiter in lithium coating experiments on HT-7 tokamak Presented by Y.J.Chen.
Fast 2-D Tangential Imaging of Edge Turbulence: Neon Mantle (draft XP) R. J. Maqueda, S. J. Zweben, J. Strachan C. Bush, D. Stutman, V. Soukhanovskii Goal:
NSTX APS-DPP: SD/SMKNov Abstract The transport properties of NSTX plasmas obtained during the 2008 experimental campaign have been studied and.
EX/P2-15 ECRH Pre-ionization and Assisted Startup in HL-2A Tokamaks in HL-2A Tokamaks Xianming SONG*, Liaoyuan CHEN, Jinghua ZHANG Jun RAO, Jun ZHOU, Xiao.
Profiles of density fluctuations in frequency range of (20-110)kHz Core density fluctuations Parallel flow measured by CHERS Core Density Fluctuations.
ASIPP Guosheng Xu EX/11-1 FEC 2012 San Diego USA 8-13 Oct. 1 Evidence of Zonal-Flow-Driven Limit-Cycle Oscillations during the L-H Transition and at H-mode.
Effects of external non-axisymmetric perturbations on plasma rotation L. Frassinetti, P.R. Brunsell, J.R. Drake, M.W.M. Khan, K.E.J. Olofsson Alfvén Laboratory,
Spontaneous rotation in stellarator and tokamak
First Experiments Testing the Working Hypothesis in HSX:
27th IAEA Fusion Energy Conference, October 2018, Gandhinagar, India
Reflectometry measurements of turbulence in Alcator C-Mod plasmas
Presentation transcript:

Toroidal rotation in ECRH L-mode, I-phase and H-mode on HL-2A tokamak A.P. Sun, J.Q. Dong, X.Y. Han, C.H. Liu, J.Y. Cao, M. Huang, Y.G. Li, X. L. Huang and J.M. Gao Southwestern Institute of Physics, China HL-2A

HL-2A Outline Introduction Charge eXchange Recombination Spectroscopy (CXRS) in HL- 2A tokamak Toroidal rotation in HL-2A experiments with co-NBI Toroidal rotation in ECRH L-mode discharges Toroidal rotation in H-mode discharges Toroidal rotation in I-phase of H-mode discharges Summary

HL-2A Introduction Plasma toroidal rotation plays a key role in regulating turbulence and has a beneficial effect on energy confinement in fusion devices. The toroidal rotation is studied on HL-2A in recent co-current direction NBI experiments and charge exchange recombination spectroscopy (CXRS) is used to measure its velocity profiles. Three cases are analyzed in this work.

HL-2A Charge exchange recombination spectroscopy in HL-2A tokamak It is in the midplace at the low magnetic field side It has 8-13 channels Its spacial resolution is 3-5cm Its time resolution is 20ms CXRS system sketch

HL-2A NBI starts at 410ms, end at 900ms. ECRH first stage start at 522ms, second stage start at 675ms, the last stage start at 828ms. Toroidal rotation in HL-2A experiments with co-NBI Toroidal rotation in ECRH L-mode discharge

HL-2A ECRH power deposition  After ECRH starts, toroidal rotation velocity decreases in the core plasma and near ECRH deposition position.  Toroidal rotation velocity changes little far away from ECRH deposition position. Toroidal rotation velocity distribution vs time

HL-2A Toroidal rotation velocity decreases significantly in the core plasma and near ECRH deposition position. Toroidal rotation velocity distribution vs R

The discharge parameters is similar to those in shot 19959, NBI and ECRH starting and ending time is the same. Toroidal rotation in ECRH L-mode discharge HL-2A

HL-2A After ECRH starts, toroidal rotation velocity decreases in the core plasma and near ECRH deposition position. Toroidal rotation velocity decreases significantly in the core plasma and near ECRH deposition position. Toroidal rotation velocity distribution vs timeToroidal rotation velocity distribution vs R

HL-2A Toroidal rotation in H-mode discharges Time evolutions of the core and edge toroidal rotation The toroidal rotation velocities increase significantly from L-mode to H-mode discharges The direction of edge toroidal rotation is reversed at the L-H transition Both core and edge toroidal rotations decrease at the H-L back transition.

HL-2A Toroidal rotation profiles in H-mode discharges The toroidal rotation continuously increases from L-mode to H-mode, and decreases from H-mode to L-mode. However, it is higher in the L-mode phase after H-L transition than that before the L-H transition. The toroidal rotation profiles at different stages The black line represents the L-mode phase. The red line does L-H transition stage. The blue line shows the beginning of the first ELM. The green line does H-mode phase. The purple line shows H-L transition stage. The yellow line represents back to L-mode stage.

HL-2A Toroidal rotation in I-phase and H-phase of H-mode discharges The toroidal rotation velocities are compared between I-phase and H-phase The stored energy increases from I- phase to H-phase. The toroidal rotation velocities in I-phase are lower than those in H-phase. The red square symbols represent I-phase the blue circular symbols do H-phase.

HL-2A Summary In ECH discharges, after ECRH starts, toroidal rotation velocity decreases significantly in the core plasma and near ECRH deposition position, and changes little far away from ECRH deposition position. In H-mode discharges, the toroidal rotation continuously increases from L-mode to H-mode, and decreases from H-mode to L-mode. However, it is larger in the L-mode phase after H-L transition than that before the L-H transition. In I-phase of H-mode discharges, the stored energy increases from I-phase to H- phase, and the toroidal rotation velocities in I-phase are lower than those in H-phase.

HL-2A Thank you for your attention!