Advanced Tokamak Plasmas and the Fusion Ignition Research Experiment Charles Kessel Princeton Plasma Physics Laboratory Spring APS, Philadelphia, 4/5/2003.

Slides:



Advertisements
Similar presentations
Glenn Bateman Lehigh University Physics Department
Advertisements

EXTENDED MHD SIMULATIONS: VISION AND STATUS D. D. Schnack and the NIMROD and M3D Teams Center for Extended Magnetohydrodynamic Modeling PSACI/SciDAC.
Physics Basis of FIRE Next Step Burning Plasma Experiment Charles Kessel Princeton Plasma Physics Laboratory U.S.-Japan Workshop on Fusion Power Plant.
ARIES-Advanced Tokamak Power Plant Study Physics Analysis and Issues Charles Kessel, for the ARIES Physics Team Princeton Plasma Physics Laboratory U.S.-Japan.
Discussion on application of current hole towards reactor T.Ozeki (JAERI) Current hole plasmas were observed in the large tokamaks of JT-60U and JET. This.
Steps Toward a Compact Stellarator Reactor Hutch Neilson Princeton Plasma Physics Laboratory ARIES Team Meeting October 3, 2002.
1 Heating and Current Drive Studies In the ARIES Program T.K. Mau University of California, San Diego Peer Review of the ARIES Program August 17, 2000.
Physics Analysis for Equilibrium, Stability, and Divertors ARIES Power Plant Studies Charles Kessel, PPPL DOE Peer Review, UCSD August 17, 2000.
Physics of fusion power
Contributions of Burning Plasma Physics Experiment to Fusion Energy Goals Farrokh Najmabadi Dept. of Electrical & Computer Eng. And Center for Energy Research.
Characteristics of Commercial Fusion Power Plants Results from ARIES-AT Study Farrokh Najmabadi Fusion Power Associates Annual Meeting & Symposium July.
Optimization of a Steady-State Tokamak-Based Power Plant Farrokh Najmabadi University of California, San Diego, La Jolla, CA IEA Workshop 59 “Shape and.
ARIES-ACT1 preliminary plasma description C. Kessel, PPPL ARIES Project Meeting, October 13, 2011.
Physics of fusion power Lecture 8 : The tokamak continued.
1 MHD for Fusion Where to Next? Jeff Freidberg MIT.
Y. Sakamoto JAEA Japan-US Workshop on Fusion Power Plants and Related Technologies with participations from China and Korea February 26-28, 2013 at Kyoto.
MHD Issues and Control in FIRE C. Kessel Princeton Plasma Physics Laboratory Workshop on Active Control of MHD Stability Austin, TX 11/3-5/2003.
TOTAL Simulation of ITER Plasmas Kozo YAMAZAKI Nagoya Univ., Chikusa-ku, Nagoya , Japan 1.
Analysis and Simulations of the ITER Hybrid Scenario C. Kessel, R. Budny, K. Indireshkumar Princeton Plasma Physics Laboratory, USA ITPA Topical Group.
1 Modeling of EAST Divertor S. Zhu Institute of Plasma Physics, Chinese Academy of Sciences.
Advanced Tokamak Regimes in the Fusion Ignition Research Experiment (FIRE) 30th Conference on Controlled Fusion and Plasma Physics St. Petersburg, Russia.
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.
Integrated Modeling and Simulations of ITER Burning Plasma Scenarios C. E. Kessel, R. V. Budny, K. Indireshkumar, D. Meade Princeton Plasma Physics Laboratory.
Advanced Tokamak Plasmas and Their Control C. Kessel Princeton Plasma Physics Laboratory Columbia University, 4/4/03.
Physics of fusion power Lecture 10: tokamak – continued.
Discussions and Summary for Session 1 ‘Transport and Confinement in Burning Plasmas’ Yukitoshi MIURA JAERI Naka IEA Large Tokamak Workshop (W60) Burning.
ITER Standard H-mode, Hybrid and Steady State WDB Submissions R. Budny, C. Kessel PPPL ITPA Modeling Topical Working Group Session on ITER Simulations.
Current Drive for FIRE AT-Mode T.K. Mau University of California, San Diego Workshop on Physics Issues for FIRE May 1-3, 2000 Princeton Plasma Physics.
TRANSP Needs for Physics Modules R. J. Hawryluk TRANSP Users Group Meeting March 24, 2015.
OPERATIONAL SCENARIO of KTM Dokuka V.N., Khayrutdinov R.R. TRINITI, Russia O u t l i n e Goal of the work The DINA code capabilities Formulation of the.
ARIES-AT Physics Overview presented by S.C. Jardin with input from C. Kessel, T. K. Mau, R. Miller, and the ARIES team US/Japan Workshop on Fusion Power.
Global Stability Issues for a Next Step Burning Plasma Experiment UFA Burning Plasma Workshop Austin, Texas December 11, 2000 S. C. Jardin with input from.
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.
Simulation and Analysis of the Hybrid Operating Mode in ITER C. Kessel, R. Budny, and K. Indireshkumar Princeton Plasma Physics Laboratory Symposium On.
OPERATIONAL SCENARIO of KTM Dokuka V.N., Khayrutdinov R.R. TRINITI, Russia O u t l i n e Goal of the work The DINA code capabilities Formulation of the.
FOM - Institute for Plasma Physics Rijnhuizen Association Euratom-FOM Diagnostics and Control for Burning Plasmas Discussion All of you.
Compact Stellarator Approach to DEMO J.F. Lyon for the US stellarator community FESAC Subcommittee Aug. 7, 2007.
D. McCune 1 PTRANSP Predictive Upgrades for TRANSP.
STUDIES OF NONLINEAR RESISTIVE AND EXTENDED MHD IN ADVANCED TOKAMAKS USING THE NIMROD CODE D. D. Schnack*, T. A. Gianakon**, S. E. Kruger*, and A. Tarditi*
ITER STEADY-STATE OPERATIONAL SCENARIOS A.R. Polevoi for ITER IT and HT contributors ITER-SS 1.
Comprehensive ITER Approach to Burn L. P. Ku, S. Jardin, C. Kessel, D. McCune Princeton Plasma Physics Laboratory SWIM Project Meeting Oct , 2007.
RFX workshop / /Valentin Igochine Page 1 Control of MHD instabilities. Similarities and differences between tokamak and RFP V. Igochine, T. Bolzonella,
PERSISTENT SURVEILLANCE FOR PIPELINE PROTECTION AND THREAT INTERDICTION International Plan for ELM Control Studies Presented by M.R. Wade (for A. Leonard)
The influence of non-resonant perturbation fields: Modelling results and Proposals for TEXTOR experiments S. Günter, V. Igochine, K. Lackner, Q. Yu IPP.
QAS Design of the DEMO Reactor
Steady State Discharge Modeling for KSTAR C. Kessel Princeton Plasma Physics Laboratory US-Korea Workshop - KSTAR Collaborations, 5/19-20/2004.
Heating and current drive requirements towards Steady State operation in ITER Francesca Poli C. Kessel, P. Bonoli, D. Batchelor, B. Harvey Work supported.
045-05/rs PERSISTENT SURVEILLANCE FOR PIPELINE PROTECTION AND THREAT INTERDICTION Taming The Physics For Commercial Fusion Power Plants ARIES Team Meeting.
Optimization of a High-  Steady-State Tokamak Burning Plasma Experiment Based on a High-  Steady-State Tokamak Power Plant D. M. Meade, C. Kessel, S.
MHD Issues and Control in FIRE C. Kessel Princeton Plasma Physics Laboratory Workshop on Active Control of MHD Stability Austin, TX 11/3-5/2003.
MCZ MCZ NCSX Mission Acquire the physics data needed to assess the attractiveness of compact stellarators; advance understanding.
18th International Spherical Torus Workshop, Princeton, November 2015 Magnetic Configurations  Three comparative configurations:  Standard Divertor (+QF)
FIRE Advanced Tokamak Progress C. Kessel Princeton Plasma Physics Laboratory NSO PAC 2/27-28/2003, General Atomics 1.0D Operating Space 2.PF Coils 3.Equilibrium/Stability.
Advanced Tokamak Modeling for FIRE C. Kessel, PPPL NSO/PAC Meeting, University of Wisconsin, July 10-11, 2001.
ZHENG Guo-yao, FENG Kai-ming, SHENG Guang-zhao 1) Southwestern Institute of Physics, Chengdu Simulation of plasma parameters for HCSB-DEMO by 1.5D plasma.
Integrated Modeling for Burning Plasmas Workshop (W60) on “Burning Plasma Physics and Simulation 4-5 July 2005, University Campus, Tarragona, Spain Under.
1PAC-37, Plasma control algorithm development on NSTX-U using TRANSP, M.D. Boyer, 1/26/2016 Dan Boyer for the Integrated Scenarios science group Plasma.
Simulation of Non-Solenoidal Current Rampup in NSTX C. E. Kessel and NSTX Team Princeton Plasma Physics Laboratory APS-DPP Annual Meeting, Savannah, Georgia,
NSTX Meeting name – abbreviated presentation title, abbreviated author name (??/??/20??) Goals of NSTX Advanced Scenario and Control TSG Study, implement,
Integrated Plasma Simulations C. E. Kessel Princeton Plasma Physics Laboratory Workshop Toward an Integrated Plasma Simulation Oak Ridge, TN November 7-9,
Presented by Yuji NAKAMURA at US-Japan JIFT Workshop “Theory-Based Modeling and Integrated Simulation of Burning Plasmas” and 21COE Workshop “Plasma Theory”
4 th General Scientific Assembly of Asia Plasma and Fusion Association (APFA) Hangzhou, China, October , 2003 AES, ANL, Boeing, Columbia U., CTD,
AES, ANL, Boeing, Columbia U., CTD, GA, GIT, LLNL, INEEL, MIT, ORNL, PPPL, SNL, SRS, UCLA, UCSD, UIIC, UWisc FIRE Collaboration FIRE.
Long Pulse High Performance Plasma Scenario Development for NSTX C. Kessel and S. Kaye - providing TRANSP runs of specific discharges S.
NIMROD Simulations of a DIII-D Plasma Disruption S. Kruger, D. Schnack (SAIC) April 27, 2004 Sherwood Fusion Theory Meeting, Missoula, MT.
Conceptual Study for the Dynamic Control of Fusion Power Plant
Features of Divertor Plasmas in W7-AS
A.D. Turnbull, R. Buttery, M. Choi, L.L Lao, S. Smith, H. St John
Influence of energetic ions on neoclassical tearing modes
New Development in Plasma and Coil Configurations
Presentation transcript:

Advanced Tokamak Plasmas and the Fusion Ignition Research Experiment Charles Kessel Princeton Plasma Physics Laboratory Spring APS, Philadelphia, 4/5/2003

What is an Advanced Tokamak? The advanced tokamak plasma simultaneously obtains –Stationary state –High plasma kinetic pressure ----> MHD stability –High self-driven current ----> Bootstrap current –Sufficiently good particle and energy confinement ----> Plasma transport –Plasma edge that allows particle and power handling ----> Boundary condition between hot core plasma and vacuum/solid walls The advanced tokamak is a recognition that the tokamak is an integrated system and requires control to succeed The advanced tokamak is a tough nut to crack

Transport Safety factor Pressure profileCurrent profile (bootstrap) LHCD, FWCD, NBCD, ECCD, HHFW NBI rotation Pellet injection Plasma shaping Impurity injection RWM feedback NTM feedback Divertor pumping plasma Ion/electron heating Alpha heating Appreciating the plasma’s integrated behavior is helping us learn to control it

Next Step Devices Must Provide the Basis for Advanced Tokamak Reactor Regime FIRE Inductive AT KSTAR FIRE AT is approaching the reactor AT regime Present tokamak experiments are pushing the envelope

Local Reduction of Energy, Particle, and Momentum Transport in Plasmas By Manipulating: Magnetic field distribution Momentum injection Electron/ion heating Current distribution Impurity injection D Pellet injection we are learning to control the location and width of the transport reduction thermal conductivity temperaturesdensity&velocity magnetic field twist centeredgeASDEX-U

Theory and Experiments Show That Powerful MHD Instabilities Can Be Controlled HBT-EP, Columbia Univ. DIII-D, General Atomics

Impurities Can Control Where Power from the Plasma is Deposited Power radiated onto high heat flux surfaces Power radiated more uniformly throughout vessel

Large Plasma Self-Driven Current Fractions are Being Attained 60-90% of the plasma current is driven by the plasma itself, from its pressure gradient ASDEX-U, Germany DIII-D,USA Japan

FIRE Has Adopted the AT Features Identified by ARIES Reactor Studies High toroidal field Double null Strong shaping Internal vertical position control coils Wall stabilizers for vertical and kink instabilities Very low toroidal field ripple ICRF/FW on-axis CD LH off-axis CD NTM stabilization from LHCD, ECCD, q>2 Tungsten divertor targets Feedback coil stabilization of RWMs Burn times exceeding current diffusion times Pumped divertor/pellet fueling/impurity control to optimize plasma edge

FIRE is Aggressively Pursuing AT Control Tools

AT Physics Control Capability on FIRE Strong plasma shaping and control Pellet injection Divertor pumping Impurity injection ICRF/FW (electron heating/CD) on-axis ICRF ion heating on/off-axis LHCD (electron heating/CD) off-axis ECCD off-axis (Ohkawa current drive) RWM MHD feedback control t(flattop)/t(curr diff) = 1-5 Diagnostics MHD J-Profile P-profile Flow-profile

FIRE Pushes to Self-Consistently Simulate Advanced Tokamak Modes 0-D Systems Analysis :Determine viable operating point global parameters that satisfy constraints Plasma Equilibrium and Ideal MHD Stability : (JSOLVER, BALMSC, PEST2, VALEN), Determine self-consistent stable plasma configurations to serve as targets Heating/Current Drive : (LSC, ACCOME, PICES, SPRUCE, CURRAY), Determine current drive efficiencies and deposition profiles Transport :(GLF23 and pellet fueling models to be used in TSC) Determine plasma density and temperature profiles consistent with heating/fueling and plasma confinement Integrated Dynamic Evolution Simulations : (Tokamak Simulation Code, WHIST, Baldur) Demonstrate self-consistent startup/formation and control including transport, current drive, fueling and equilibrium Edge/SOL/Divertor :(UEDGE) Find self-consistent solutions connecting the core plasma with the divertor

FIRE AT Integrated Simulations Show Attractive Features Q ≈ 5

Advanced Tokamaks --- We Want to Have It Our Way The advanced tokamak is characterized by the features we need for a viable fusion power plant Access to this regime requires control of the plasma and we are learning how by penetrating its coupled physics FIRE is a next step burning plasma device –Utilizing experimental advanced tokamak accomplishments –Adopting design features of advanced tokamak reactor designs –Applying integrated simulation tools to project the advanced tokamak performance FIRE can bridge the AT physics gap from present experiments to the reactor regime