Electromagnetic Particle Injector (EPI) Proposed as a Backup Disruption Mitigation System for ITER The EPI system accelerates a sabot to high-velocity.

Slides:



Advertisements
Similar presentations
1 Primary Research of Massive Gas Injection for Disruptions Mitigation on HT-7 H.D. Zhuang X.D. Zhang Y.Zhang Institute of Plasma Physics. CAS
Advertisements

Stereotype threat is defined as the experience of anxiety when faced with a confirmable stereotype (Steele & Aronson, 1995). Often anxiety obstructs cognitive.
Sediment Movement after Dam Removal
Beta decay and Structure of Exotic Nuclei near 78 Ni Alexander Lisetskiy NSCL,JINA,MSU.
Runaway Electron Mitigation Collaboration on J-TEXT David Q. Hwang UC Davis Sixth US-PRC Magnetic Fusion Collaboration Workshop Collaborating Institutions:
ATLAS LHCf Detector 140m away from the interaction point LHCf: calibration of hadron interaction models for high energy cosmic-ray physics at the LHC energy.
PHYS 101 Knight et al. – ch. 1. Which car is going faster ?
Further Study of Ion Pickup. Turbulent Alfven waves and magnetic field lines Turbulent waves represent enhanced random fluctuations. Fluctuations vitiate.
CE 230-Engineering Fluid Mechanics
Magnetic Reconnection Rate and Energy Release Rate Jeongwoo Lee 2008 April 1 NJIT/CSTR Seminar Day.
The MERIT experiment at the CERN PS Leo Jenner MOPC087 WEPP169 WEPP170.
Enter SK / KD / Indicators. Discovered Corpuscles/Electrons in 1897 picture.
Acceleration. MEANING FORMULA = A = Acceleration V f = V i = t=
Measuring Water in Motion and Motion in Water RD Instruments Home of the ADCP Channel Master HADCP.
Ronald Petzoldt, Dan Goodin, Brian Vermillion, Neil Alexander, Tom Drake, Bob Stemke, Lane Carlson, Landon Carlson Presented by Daniel Frey High Average.
Raman, BPW (W60) 4-5 July 2005 Advanced fueling system for use as a burn control tool Roger Raman University of Washington, Seattle Workshop (W60) on Burning.
Raman,11 STW 3-6 Oct 2005 Fueling Requirements for Steady State Spherical Torus Operation Roger Raman, Thomas R. Jarboe, + Henry W. Kugel University of.
Recent JET Experiments and Science Issues Jim Strachan PPPL Students seminar Feb. 14, 2005 JET is presently world’s largest tokamak, being ½ linear dimension.
NSTX-U PCTF Pre-Forum Meeting – Boron Carbide Injection, Lunsford (1/20/2015) Granular Boron Carbide triggered ELM events within Boronized Discharges Identify.
1 Critical Need for Disruption PAM in Tokamaks (FESAC 2014): S.A. Sabbagh, N. Commaux, N. Eidietis, S.P. Gerhardt, et al. (July 9 th, 2014) Critical Need.
V. A. Soukhanovskii NSTX Team XP Review 31 January 2006 Princeton, NJ Supported by Office of Science Divertor heat flux reduction and detachment in lower.
Update on IFE Target Fabrication and Injection Activities Presented by Dan Goodin at the ARIES Project Meeting January 10-11, 2002 UCSD San Diego, California.
V. A. Soukhanovskii 1 Acknowledgement s: R. Maingi 2, D. A. Gates 3, J. Menard 3, R. Raman 4, R. E. Bell 3, C. E. Bush 2, R. Kaita 3, H. W. Kugel 3, B.
1 Materials Science Concepts MATS-535 Electronics and Photonics Materials Scope a – Atomic Structure and Atomic Number b – Bonding and Type of Solids Dr.
Fast liquid Lithium “shower” injector G. A. Wurden Los Alamos NSTX Brainstorming Meeting Feb 7-8, 2012.
Status of Target Injector and In-Chamber Tracking Ronald Petzoldt, Dan Goodin, Neil Alexander, Gottfried Besenbruch, Tom Drake, Brian Vermillion, Bob Stemke,
H. W. Kugel 45 th APS DPP Meeting Oct 27-31, 2003, Albuquerque, NM 1 Lithium Experiments in the NSTX Boundary Physics Program H.W.Kugel, M.Bell, R.Kaita,
The executive summary.
Behaviour of Runaway Electrons during Injection of High Z Impurities/Gas Puffing in HT-7 S.Sajjad INSTITUTE OF PLASMA PHYSICS,HEFEI CHINA.
5.5 inch 8 inch 6 inch V = m/s Freq = Hz Independent Control:
Europa Penetrator Design and Survivability Testing IPPW10 Sanjay Vijendran, ESA ESTEC Marie-Claire Perkinson, Lester Waugh, Mike Williams, Astrium Tom.
CST Particle studio. Analysis of “STEP-OUT” Olav Berrig Thanks to Benoit Salvant.
TRANSP for core particle transport studies M. Maslov.
T. Bolzonella – 9 February 2011 – RFX-mod programme workshop TF1: Physics integration for high performance RFP Proposals and discussion T. Bolzonella,
5.5: Speeding up and Slowing down
Design of an Inertial Fusion Energy Target Injection & Tracking System Ronald Petzoldt, Dan Goodin, Mike Hollins, Chuck Gibson, Neil Alexander, and Gottfried.
V. A. Soukhanovskii Lawrence Livermore National Laboratory H. W. Kugel, R. Kaita, A. L. Roquemore Princeton Plasma Physics Laboratory NSTX Research Team.
Sensory Receptors: Transduction and Coding Narrado por: Renato M.E. Sabbatini, PhD.
LIU Beam Parameter Working Group Meeting #1: Ion parameter table Outline: Where we are standing What we need to do (still in 2015)
Physics 213 General Physics Lecture Exam 3 Results Average = 141 points.
Acceleration Acceleration is the rate of change of velocity.
Tuomas Tala 1/16 ITPA TC Meeting, Princeton, USA 5 October – 7 October 2009 T. Tala (JET, DIII-D), W. Solomon (DIII-D, JET, NSTX) and S. Kaye, L.F. Delgado-
Disruption Mitigation System Developments and Design for ITER L.R. Baylor, C. Barbier, N.D. Bull, J.R. Carmichael, M.N. Ericson, M.S. Lyttle, S.J. Meitner,
 Matter is any thing that occupies space & has mass  Present in three states: solid, liquid, & gas  It could be divided into elements & compounds 
The Atomic Models of Thomson and Rutherford Rutherford Scattering The Classic Atomic Model The Bohr Model of the Hydrogen Atom Successes & Failures of.
Chapter 5 Agile Development Moonzoo Kim KAIST
Chapter 13 Gravitation In this chapter we will explore the following topics: -Newton’s law of gravitation, which describes the attractive force between.
Lecture 19 Electromagnetic Waves.
NSTX-U Supported by Fast Time Response Electromagnetic Particle Injection Concept for Disruption Mitigation (EPI) 1R. Raman, 1T.R. Jarboe, 2J.E. Menard,
Magnetism Magnetism Lecture 15 Today Magnetic Fields
Nature Of Light & Electromagnetic Spectrum
First results from IS468 and further investigation of in-trap decay of 62Mn First results from 2008 ; Problems and questions ; Further investigations ;
Hypervelocity Impact Measurements and Simulations
Modified Design of Aries T-Tube Divertor Concept
Wet Granulation Small Scale Experiments
Find the velocity of a particle with the given position function
Graphing Motion Walk Around
CONTROL OF VOLTAGE PLASMA OSCILLATIONS IN A DC
Acceleration.
Find the velocity of a particle with the given position function
Introduction to fractional Brownian Motion for Terrain
SOL plasma in ITER is dense and hot  thick to gas puff as in C-mod
TPF = max(Prad(fn=1)) /Prad(fn=1)
One Transport v4 Migration Update
Production Cross-Sections of Radionuclides in Proton- and Heavy Ion-Induced Reactions Strahinja Lukić.
Vectors - Doing basic physics with vectors Contents:
Table 2. Air-water flow cases
EX/P7-12, R&D for reliable disruption mitigation in ITER, M
a = v2 – v1 t a = 8 m/s s a = 8 m/s2 a = 36 m/s – 4 m/s 4 s #6 d
Fig. 1 Schematic depiction of a paradigm for rapid and guided discovery of materials through iterative combination of ML with HiTp experimentation. Schematic.
Presentation transcript:

Electromagnetic Particle Injector (EPI) Proposed as a Backup Disruption Mitigation System for ITER The EPI system accelerates a sabot to high-velocity using an electromagnetic impeller At the end of the acceleration, within 2-3ms, the sabot will release granules of known velocity and distribution – or a Shell Pellet The primary advantage of the EPI concept over SPI and other gas propelled systems is its potential to meet short warning time scales, while accurately delivering the required particle size and materials at the velocities needed for achieving the required core penetration (into the RE channel) in high power ITER discharges. Experimental Confirmation of Rapid Response Time and Velocity that is consistent with projections University of Washington / PPPL R. Raman, et al., FIP/P1-51