Interplay between magnetic topology, density fluctuations and confinement in high-  Wendelstein 7-AS plasmas Nils P. Basse 1 Association EURATOM – Risø.

Slides:



Advertisements
Similar presentations
TEC Trilateral Euregio Cluster Institut für PlasmaphysikAssoziation EURATOM-Forschungszentrum Jülich IEA Large Tokamak IA Workshop on Edge Transport in.
Advertisements

9th TTF Spain September 11, 2002 B. J. Peterson, NIFS, Japan page 1 Radiative Collapse and Density Limit in the Large Helical Device.
Fig.11_ctrlcoil [W7ASrev_11_ctrlcoil] Effect of control coils (B = 1.25 T,  vac = 0.52, P NBI = 3.1 MW). (a) A significant increase of the stored energy.
FOM-Institute for Plasma Physics Rijnhuizen Association Euratom-FOM, Trilateral Euregio Cluster Feedback controlled ECRH power deposition for control of.
Sub-THz Component of Large Solar Flares Emily Ulanski December 9, 2008 Plasma Physics and Magnetohydrodynamics.
Results from Visible Light Imaging of Alfvén Fluctuations in the H-1NF Heliac J. Read, J. Howard, B. Blackwell, David Oliver, & David Pretty Acknowledgements:
Physics of fusion power
13th IEA/RFP Workshop – Stockholm October 9-11, D characterization of thermal core topology changes in controlled RFX-mod QSH states A. Alfier on.
Physics of fusion power Lecture 8 : The tokamak continued.
MCZ Equilibrium and Stability of High-  Plasmas in Wendelstein 7-AS M.C. Zarnstorff 1, A. Weller 2, J. Geiger 2, E. Fredrickson 1, S. Hudson.
Magnetic Reconnection Rate and Energy Release Rate Jeongwoo Lee 2008 April 1 NJIT/CSTR Seminar Day.
Physics of fusion power Lecture 10 : Running a discharge / diagnostics.
SUMMARY OF EXPERIMENTAL CORE TURBULENCE CHARACTERISTICS IN OH AND ECRH T-10 TOKAMAK PLASMAS V. Vershkov, L.G. Eliseev, S.A. Grashin. A.V. Melnikov, D.A.
A. HerrmannITPA - Toronto /19 Filaments in the SOL and their impact to the first wall EURATOM - IPP Association, Garching, Germany A. Herrmann,
Fast imaging of global eigenmodes in the H-1 heliac ABSTRACT We report a study of coherent plasma instabilities in the H-1 plasma using a synchronous gated.
1 ST workshop 2008 Conception of LHCD Experiments on the Spherical Tokamak Globus-M O.N. Shcherbinin, V.V. Dyachenko, M.A. Irzak, S.A. Khitrov A.F.Ioffe.
Nils P. Basse Plasma Science and Fusion Center Massachusetts Institute of Technology Cambridge, MA USA ABB seminar November 7th, 2005 Measurements.
pkm- NCSX CDR, 5/21-23/ Power and Particle Handling in NCSX Peter Mioduszewski 1 for the NCSX Boundary Group: for the NCSX Boundary Group: M. Fenstermacher.
Interplay between confinement, turbulence and magnetic topology Nils P. Basse, S. Zoletnik 1, W. L. Rowan 2 et al. MIT Plasma Science and Fusion Center.
Plasma Dynamics Lab HIBP E ~ 0 V/m in Locked Discharges Average potential ~ 580 V  ~ V less than in standard rotating plasmas Drop in potential.
12/03/2013, Praga 1 Plasma MHD Activity Observations via Magnetics Diagnostics: Magnetic island Analysis Magnetic island Analysis Frederik Ostyn (UGent)
Physics of fusion power Lecture 10: tokamak – continued.
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.
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.
Physics of fusion power Lecture 9 : The tokamak continued.
14 Oct. 2009, S. Masuzaki 1/18 Edge Heat Transport in the Helical Divertor Configuration in LHD S. Masuzaki, M. Kobayashi, T. Murase, T. Morisaki, N. Ohyabu,
N. Fedorczak O-26 PSI 2010 San Diego 1 Nicolas Fedorczak Poloidal mapping of turbulent transport in SOL plasmas. G. Bonhomme,
EAST Data processing of divertor probes on EAST Jun Wang, Jiafeng Chang, Guosheng Xu, Wei Zhang, Tingfeng Ming, Siye Ding Institute of Plasma Physics,
DIII-D SHOT #87009 Observes a Plasma Disruption During Neutral Beam Heating At High Plasma Beta Callen et.al, Phys. Plasmas 6, 2963 (1999) Rapid loss of.
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.
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.
M. Onofri, F. Malara, P. Veltri Compressible magnetohydrodynamics simulations of the RFP with anisotropic thermal conductivity Dipartimento di Fisica,
Temporal separation of turbulent time series: Measurements and simulations Nils P. Basse 1,2, S. Zoletnik, M. Saffman, G. Antar, P. K. Michelsen and the.
Transport in three-dimensional magnetic field: examples from JT-60U and LHD Katsumi Ida and LHD experiment group and JT-60 group 14th IEA-RFP Workshop.
ASIPP HT-7 The effect of alleviating the heat load of the first wall by impurity injection The effect of alleviating the heat load of the first wall by.
HL-2A Jiaqi Dong Southwestern Institute of Physics & Institute for Fusion Theory and Simulation, ZJU International West Lake Workshop on Fusion Theory.
Measurements of plasma turbulence by laser scattering in the Wendelstein 7-AS stellarator Nils P. Basse 1,2, S. Zoletnik, M. Saffman, P. K. Michelsen and.
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al. Sawtooth-like phenomena in LHD S. Ohdachi, S.Yamamoto, K. Toi, K. Y.Watanabe, S.Sakakibara,
TEC Trilateral Euregio Cluster Institut für PlasmaphysikAssoziation EURATOM-Forschungszentrum Jülich 21st IAEA Fusion Energy Conference, October.
Effect of Helical Magnetic Field Ripples on Energetic Particle Confinement in LHD Plasmas T.Saida, M.Sasao, M.Isobe 1, M.Nishiura 1, S.Murakami 2, K.Matsuoka.
The influence of non-resonant perturbation fields: Modelling results and Proposals for TEXTOR experiments S. Günter, V. Igochine, K. Lackner, Q. Yu IPP.
MCZ Active MHD Control Needs in Helical Configurations M.C. Zarnstorff 1 Presented by E. Fredrickson 1 With thanks to A. Weller 2, J. Geiger 2,
Role of thermal instabilities and anomalous transport in the density limit M.Z.Tokar, F.A.Kelly, Y.Liang, X.Loozen Institut für Plasmaphysik, Forschungszentrum.
18th International Spherical Torus Workshop, Princeton, November 2015 Magnetic Configurations  Three comparative configurations:  Standard Divertor (+QF)
47th Annual Meeting of the Division of Plasma Physics, October 24-28, 2005, Denver, Colorado ECE spectrum of HSX plasma at 0.5 T K.M.Likin, H.J.Lu, D.T.Anderson,
Interplay between confinement, turbulence and magnetic topology Nils P. Basse MIT Plasma Science and Fusion Center This proposal originates from density.
Plasma MHD Activity Observations via Magnetic Diagnostics Magnetic islands, statistical methods, magnetic diagnostics, tokamak operation.
Development and Assessment of “X-point limiter” Plasmas M. Bell, R. Maingi, K-C. Lee Coping with both steady-state and transient (ELM) heat loads is a.
Initial Results from the Scintillator Fast Lost Ion Probe D. Darrow NSTX Physics Meeting February 28, 2005.
Presented by Yuji NAKAMURA at US-Japan JIFT Workshop “Theory-Based Modeling and Integrated Simulation of Burning Plasmas” and 21COE Workshop “Plasma Theory”
Plasma Turbulence in the HSX Stellarator Experiment and Probes C. Lechte, W. Guttenfelder, K. Likin, J.N. Talmadge, D.T. Anderson HSX Plasma Laboratory,
HT-7 Proposal of the investigation on the m=1 mode oscillations in LHCD Plasmas on HT-7 Exp2005 ASIPP Youwen Sun, Baonian Wan and the MHD Team Institute.
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.
Hard X-rays from Superthermal Electrons in the HSX Stellarator Preliminary Examination for Ali E. Abdou Student at the Department of Engineering Physics.
Dominik Schega (1), S.S.Abdullaev (1), M.Clever (1), K.H.Finken (1), M.Jakubowski (2), Y.Kikuchi (3), M.Lehnen (1), O.Schmitz (1), G.Sewell (4), H.Stoschus.
1 Edge Characterization Experiment in High Performance (highly shaped) Plasmas R. J. Maqueda (Nova Photonics) R. Maingi (ORNL) V. Soukhanovskii (LLNL)
NIMROD Simulations of a DIII-D Plasma Disruption S. Kruger, D. Schnack (SAIC) April 27, 2004 Sherwood Fusion Theory Meeting, Missoula, MT.
Member of the Helmholtz Association Meike Clever | Institute of Energy Research – Plasma Physics | Association EURATOM – FZJ Graduiertenkolleg 1203 Dynamics.
48th Annual Meeting of the Division of Plasma Physics, October 30 – November 3, 2006, Philadelphia, Pennsylvania Energetic-Electron-Driven Alfvénic Modes.
48th Annual Meeting of the Division of Plasma Physics, October 30 – November 3, 2006, Philadelphia, Pennsylvania HIBP Designs for Measurement of the Electric.
Mechanisms for losses during Edge Localised modes (ELMs)
T. Markovič1,2, P. Cahyna1, R. Panek1, M. Peterka1,2, P. C
in tokamaks and stellarators
Investigation of triggering mechanisms for internal transport barriers in Alcator C-Mod K. Zhurovich C. Fiore, D. Ernst, P. Bonoli, M. Greenwald, A. Hubbard,
NATIONAL RESEARCH CENTER “KURCHATOV INSTITUTE”
20th IAEA Fusion Energy Conference,
Reflectometry measurements of turbulence in Alcator C-Mod plasmas
Ioffe Summary Fast MHD oscillations observed on the TUMAN-3M in absence of energetic ions Bursts of the oscillations correlate with saw-tooth crashes and.
Presentation transcript:

Interplay between magnetic topology, density fluctuations and confinement in high-  Wendelstein 7-AS plasmas Nils P. Basse 1 Association EURATOM – Risø National Laboratory, Denmark 2 Ørsted Laboratory, Niels Bohr Institute for Astronomy, Physics and Geophysics, Denmark 1. Discharge overview 2. Magnetic topology 3. Density fluctuations 4. Conclusions

Discharge overview Basic parameters: Edge rotational transform  a = 0.41, B tor = T and P NBI = 4 MW Scan of plasma current I p = 0 (solid), -2 (dotted) and -4 (dashed) kA Negative/positive frequencies are due to inward/outward moving fluctuations, respectively

Magnetic topology Visible radiation (Jürgen Baldzuhn & Andreas Werner) Left-hand (outboard) structures are control coils, top/bottom right-hand (inboard) elements are divertor parts As  a increases, the plasma edge exhibits a smooth  island  ergodic transition

Magnetic topology Finite-  calculations (Joachim Geiger) The reconfiguring of the neutral beam injection system allowed us to obtain a record of 3.1 % The NEMEC code enables the calculation of finite-  flux surfaces, but cannot handle natural magnetic islands

Magnetic topology Natural 5/m islands (Andreas Werner) The Gourdon code can be used to study magnetic islands, but only for vacuum An increase of  a leads to island chains having a decreasing m number

Density fluctuations Reflectometry (Jaco van Gorkom) Density fluctuations in rotating MHD- modes have been investigated in TEXTOR Density fluctuations inside an O- point are larger than those behind the X-point EPS 2001 Behind X-point Inside O-point

Density fluctuations Autopower spectra (3D) Positive frequency fluctuations decrease/increase at high/low frequencies with increasing current Negative high frequency component disappears completely Negative low frequency component remains at a constant level

Density fluctuations Autopower spectra (2D) Left-hand plot: Initial plasma phase, all spectra identical Right-hand plot: Later high-  phase; note the pronounced decrease of high frequency fluctuations, especially for negative frequencies

Conclusions The investigation of density fluctuations in high-  plasmas was triggered by the interesting phenomena seen in TEXTOR In the work presented we have assumed that natural islands in W7-AS behave similarly to MHD-islands in TEXTOR If this is indeed the case, our observations can be explained as follows: 1. An O-point is observed in the early phase for positive frequencies 2. Later, what seems to be an O- to X-point transition occurs for negative frequencies 3. O-point at the bottom, O- to X-point transition at the top (assuming that high frequency fluctuations travel in the electron diamagnetic drift direction) 4. The observed island chain is probably 5/12 (12 islands in a poloidal cross section) 5. Asymmetry is likely to be due to the flux surface tilt at the diagnostic position