No Li 130374 130386 130388 130389 No Li 47 mg 5 mg/s 10 mg/s.

Slides:



Advertisements
Similar presentations
2 nd ISLAFD, April , Princeton NJ Nuclear, Plasma, and Radiological Engineering Center for Plasma-Material Interactions Contact:
Advertisements

XP 1157 Increasing the CHI start-up current magnitude in NSTX B.A. Nelson et al. 1.
ASIPP Characteristics of edge localized modes in the superconducting tokamak EAST M. Jiang Institute of Plasma Physics Chinese Academy of Sciences The.
ASC XP-823 Error Field Correction and Long Pulse J.E. Menard, S.P. Gerhardt Part 1 Determine the source of, and optimal correction for, the observed n=3.
Lithium Free-Surface Flow and Wave Experiments H.Horiike 1), H.Kondo 1), H.Nakamura 2), S.Miyamoto 1), N.Yamaoka 1), T.Muroga 3) 1) Graduate School of.
Lithium Surface Experiments on the Current Drive Experiment-Upgrade R. Kaita Princeton Plasma Physics Laboratory National Spherical Torus Experiment Program.
ASIPP Lithium experiments on HT-7 and EAST tokamak G. Z. Zuo, J. S. Hu, Z.S, J. G. Li, EAST team Institute of Plasma Physics, Chinese Academy of Sciences,
Wireless Underwater Power Transmission (WUPT) for Lithium Polymer Charging James D’Amato Shawn French Warsame Heban Kartik Vadlamani December 5, 2011 School.
Assessment of beam-target interaction of IFMIF A state of the art J. Knaster a, D. Bernardi b, A. García c, F. Groeschel h, R. Heidinger d, M. Ida e, A.
Development of a mover having one nanometer precision and 4mm moving range Y. Morita, S. Yamashita ICEPP, University of Tokyo Y. Higashi, M. Masuzawa,
LIGO-G0200XX-00-M LIGO Laboratory1 Pre-Isolation Dennis Coyne LIGO Laboratory NSF LIGO Annual Review, at MIT 23 October 2002.
1 Sinusoidal Waves The waves produced in SHM are sinusoidal, i.e., they can be described by a sine or cosine function with appropriate amplitude, frequency,
A. Canton, S. Dal Bello 13 th IEA/RFP Workshop Density control in RFX-mod A. Canton, S. Dal Bello Consorzio RFX, Padova, Italy.
XP810 and 801 report, Feb 08 slide 1 Buttery, Gerhardt, La Haye, Sabbagh June 2008 reporting meeting – XP810 and 801 experiment: 801: Marginal island width.
ILE, Osaka Concept and preliminary experiment on protection of final optics in wet-wall laser fusion reactor T. Norimatsu, K. Nagai, T. Yamanaka and Y.
November 22, 2005 Physical Pendulum Pivot disk about a point a distance h from the center; What is the period T of oscillation? h mg   Find  (t) for.
Simple Harmonic Motion
9/20/04NSTX RESULTS REVIEW NSTX rtEFIT implementation progress results NSTX 2004 RESULTS REVIEW September 20&21, 2004 REAL-TIME EQUILIBRIUM RECONSTRUCTION.
Introduction A lightweight film known as Kapton with 12 piezoelectric transducers attached was subjected to a frequency range of 1 kHz to 15 MHz of current.
Acousto optic modulators Additional details relevant for servos.
NSTX S. A. Sabbagh XP501: MHD spectroscopy of wall stabilized high  plasmas  Motivation  Resonant field amplification (RFA) observed in high  NSTX.
Development of Tungsten Injection System for High Z Impurity Transport Study in KSTAR Hyun Yong Lee 1,2 *, Suk-Ho Hong 3, Joohwan Hong 1,2, Seung Hun Lee.
ASIPP Development of a new liquid lithium limiter with a re-filling system in HT-7 G. Z. Zuo, J. S. Hu, Z.S, J. G. Li,HT-7 team July 19-20, 2011 Institute.
V. A. Soukhanovskii 1 Acknowledgements: M. G. Bell 2, R. Kaita 2, H. W. Kugel 2, R. Raman 3, A. L. Roquemore 2 1 Lawrence Livermore National Laboratory,
HT-7 Lithium coating and its influence on plasma performance on HT-7 Z. Sun, J.S. Hu, G.Z. Zuo, J.G. Li ASIPP
1 CHI Summary Transient CHI (XP606) –All systems operated reliably without any faults Edge Current drive (XP533)
Mid-Run Assessment - ISD S. Kaye, D. Gates 10 May 2006.
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.
Flows, Turbulence, and the Edge Plasma in NSTX C.E. Bush, S. Zweben, R. Maqueda, W. Davis, D. Johnson, R. Kaita, H. Kugel, L. Roquemore, G. Wurden and.
1Physics Operators Course, PCS Navigation, D.J. Battaglia, September 15, 2015 Devon Battaglia, Keith Erickson, Dennis Mueller, Stefan Gerhardt, Roger Raman,
NSTX-U NSTX-U PAC-31 Response to Questions – Day 1 Summary of Answers Q: Maximum pulse length at 1MA, 0.75T, 1 st year parameters? –A1: Full 5 seconds.
Centrifugal Li Granule Injection (Can Injected Lithium Granules Trigger ELMs?) D.K. Mansfield, A.L. Roquemore, H.K. Kugel (PPPL), L.R. Baylor, R. Maingi.
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,
2 The Neutral Particle Analyzer (NPA) on NSTX Scans Horizontally Over a Wide Range of Tangency Angles Covers Thermal ( keV) and Energetic Ion.
Advances In High Harmonic Fast Wave Heating of NSTX H-mode Plasmas P. M. Ryan, J-W Ahn, G. Chen, D. L. Green, E. F. Jaeger, R. Maingi, J. B. Wilgen - Oak.
Integration and Plasma Control D.A. Gates, M.G. Bell NSTX 5-Year Plan June 30-July 2, 2003.
CHI Run Summary for March 10-12, 31 & April 9, 2008 Flux savings from inductive drive of a Transient CHI started plasma (XP817) R. Raman, B.A. Nelson,
Measurements of dust movement by fast TV camera in JT-60U Nobuyuki Asakura, H.Kawashima, N.Ohno 1), T.Nakano, S.Takamura 2), Y.Uesugi 3) 1) Japan Atomic.
PXL vibration and stability 1/7/2014. Measurements of: Cooling air induced vibration of the PXL sensors as a function of air flow DC position change as.
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.
Yb:YAG Regenerative Amplifier for A1 Ground Laser Hut Rui Zhang ACCL Division V, RF-Gun Group Nov 20, 2015 SuperKEKB Injector Laser RF Gun Review.
5.5 inch 8 inch 6 inch V = m/s Freq = Hz Independent Control:
HL-2A Heating & Current Driving by LHW and ECW study on HL-2A Bai Xingyu, HL-2A heating team.
FEC 2006 Reduction of Neoclassical Transport and Observation of a Fast Electron Driven Instability with Quasisymmetry in HSX J.M. Canik 1, D.L. Brower.
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.
NCSX NCSX CDR May 21-23, 2002 H.W. Kugel Slide 1 Conceptual Design for NCSX Auxiliary Systems Heating, Fueling,Wall Conditioning and Vacuum Systems.
Solenoid Free Plasma Start-up Mid-Run Summary (FY 2008) R. Raman and D. Mueller Univ. of Wash. / PPPL 16 April 2008, PPPL 1 Supported by Office of Science.
Scattering Control using COMSOL Multiphysics Modeling Billy D. Jones APL-UW 4 Feb 2016.
M. Ono NSTX FWP 2014 Budget Planning Meeting Apr. 15, 2012 Chapter 10. NSTX-U Facility Status and Proposed Upgrades Text, figures – mostly there except.
Biased Electrode Experiment S.J. Zweben, R.J. Maqueda, L. Roquemore, R.J. Marsala, Y. Raitses, R. Kaita, C. Bush R.H. Cohen, D.D. Ryutov, M. Umansky (LLNL)
V. A. Soukhanovskii Lawrence Livermore National Laboratory H. W. Kugel, R. Kaita, A. L. Roquemore Princeton Plasma Physics Laboratory NSTX Research Team.
SMK – XP 1 XP 811: Effect of Rotation on Energy/Impurity Confinement S. Kaye, L. Delgado-Aparicio Joule Milestone Description –XP directly addresses Joule.
Supported by Office of Science NSTX S.M. Kaye, PPPL ITPA PPPL 5-7 Oct Confinement and Transport in NSTX: Lithiumized vs non-Lithiumized Plasmas Culham.
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.
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.
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,
NSTX APS-DPP: SD/SMKNov Abstract The transport properties of NSTX plasmas obtained during the 2008 experimental campaign have been studied and.
Long Pulse High Performance Plasma Scenario Development for NSTX C. Kessel and S. Kaye - providing TRANSP runs of specific discharges S.
1 Edge Characterization Experiment in High Performance (highly shaped) Plasmas R. J. Maqueda (Nova Photonics) R. Maingi (ORNL) V. Soukhanovskii (LLNL)
For the NSTX Five-Year Research Program 2009 – 2013 M.G. Bell Facility and Diagnostic Plans.
Reconnection Process in Sawtooth Crash in the Core of Tokamak Plasmas Hyeon K. Park Ulsan National Institute of Science and Technology, Ulsan, Korea National.
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,
Date of download: 10/9/2017 Copyright © ASME. All rights reserved.
Reduction of ELM energy loss by pellet injection for ELM pacing
Measuring the Dynamics of Injected Boron Dust Particles in the Scrape-Off Layer Aaron Bader Dec 14, 2006 Ideas Forum 2007.
Acoustic Upside-down Levitator With A Solid Sample
ELMs and plasma-materials interactions mitigated with flowing lithium PFCs and active lithium injection in EAST 3rd generation flowing liquid lithium.
Xiao-Bo Wang, Jody Vykoukal, Frederick F. Becker, Peter R.C. Gascoyne 
Li I light from DiMES during locked mode (Dt ~ 16 ms)
Presentation transcript:

No Li No Li 47 mg 5 mg/s 10 mg/s

All eleven shots technically successful – small timing problem Ramp-ups and square wave temporal profiles employed Rates from 1 mg/s to ~ 35 mg/s employed NSTX much more tolerant of Li powder than expected Total of 82 mg injected during 11 shots Not a great day for NSTX reproducibility or documentation shots have some scientific merit Observed significant decrease in D  and ELMs Timing and location of deposition appeared to be important XP-828 Initial Results and Observations

Extra Slides

Prototype Acoustic Resonance Dropper Can Drop from 0.3 mg up to Much-Too-Much Powder (Li Surrogate) Velocity at SOL = 4.5 m/sec Powder Injector

to Vac Pump 1.0 m 2 ¾ Gate Valve Laser Scattering Module Drop Chamber Bracing ½ O.D. Stainless Tubing Pyrex Tube 2 ½ O.D. Glass Funnel w Long Stem to Vac Pump Existing Computerized Laboratory Test Facility

New Umbrella Throttle Seems to Work More Reliably Than Old Simple Throttle Design – Higher Fluxes Simple ThrottleUmbrella Throttle Higher Reliable Particle Flow Li Powder Li Powder (~ 3 mg/s)

RMS Voltage (Volts) Mass Flux (mg/s) Lithium Particle Flux is an Approximately Linear Function of Resonant Voltage Applied to the Piezoelectric Membrane

Scattered Laser Signal (A.U.) Time (s) 0.5 V: 0.4 mg/s 1.0 V: 0.7 mg/s 2.0 V: 1.5 mg/s 3.0 V: 2.2 mg/s 8.0 V: 5.8 mg/s Laser Scattered Signal Reproducibility is Fairly Good However, Signal Saturates at mg/s (3 - 5 Vrms)

Time (s) RMS Voltage (Volts) Scattered Laser Signal (A.U.) Two Arbitrary Waveforms: Ramp-Ups (4 & 8 Volts Max) Laser Scattered Signal Saturates at mg/s (3 - 5 Vrms) 6 mg/s 3mg/s

Time (s) RMS Voltage (Volts) Scattered Laser Signal (A.U.) 6 mg/s Arbitrary Waveform: Ramp-Down (8 Volts Max) Same Laser Scattering Saturation Observed

RMS Voltage (Volts) Time (s) Scattered Laser Signal (A.U.) 6 mg/s An Arbitary Waveform: With Some Modifications Might “Tweek” ELMS

“Early” Li Can be Preferentially Directed to Lower Divertor Pre-Pulse of Lithium for 50 ms (~ 100 Oscillations) 850 ms Before Breakdown Small Plasma Initiated on the Center Stack Flux Plot Shown Just After Breakdown

The Two Plasmas to be Used in XP

XP828 Shot No. Dropper mg/s (Max) Temporal Profile Total Lithium (mg) HeGDC (min) Ref #10N/A06 Ref #20N/A06 Ref #30N/A06 13A26 26A66 312A or TBDA or TBDB or TBDB or TBDB or TBDB or TBDC or TBDC or TBDC TBD TBD TBD TBD

Plasma Current Time (sec) Li Flux 01 Pre-programmed Flux Profile Must be Injected ~ 450 ms Before Plasma Breakdown 450 ms

NewDiff 1.05FitX_v() 80VoltX_v 

B T = 0.5 T I p = 800 kA Purpose : Study ELM Suppression by in situ Modification of NSTX Plasma Surface Interaction: Li on Graphite R/a = 1.46 Lower Single Null P NBI = 4 MW Type 1 ELMS Lithium Evaporators with Shutters H. Kugel P2-58 B treated Graphite 2

Velocity at SOL = 4.5 m/sec Powder Injector

Dropper by Acoustic Resonance Vertical Injection by Acoustic Resonance Horizontal Injection by PZT Fan

100  m Resonating Piezoelectric Disk SLMP Li Powder  Resonant Levitation = ± 0.5 mm ~ 5 lbs

0,1 Mode 290 Hz 0,2 Mode 2 kHz 0,3 Mode Modes of the Vibrating Piezoelectric Drumhead

0,2 Mode of Piezoelectric Disk with Glass Beads – 2 KHz

0,2 Node of Piezoelectric Disk with Glass Beads – 2 KHz

30 mil Scale 20:1 Throttle: ¼ - 28 Screw Piezoelectric Membrane (0,2) Node 3.5 mg/s 0.3 mg/s mg/s g Fixed Level Inside Node N.B. 30mil Gap: 15 particles high 20 particles wide O-Ring 100 mil

Resonating Piezoelectric Disk  Resonant Levitation 25 mm (0,2) Mode Dusting of Glass Spheres Levitated from Center of Mode Throttle used to force Particles to drop through Hole in piezo membrane

Dropper by Acoustic Resonance Vertical Injection by Acoustic Resonance Horizontal Injection by PZT Fan (or by Rotating Wheel)