Dynamic Resonant Error Field Correction with C-COIL and I-COIL in the DIIID device
|
|
- Sherilyn Day
- 6 years ago
- Views:
Transcription
1 Dynamic Resnant Errr Field Crrectin with C-COIL and I-COIL in the DIIID device M. Okabayashi, M.S. Chance, R, Hatcher, J. Manickam P P P L, J. Bialek, A.M. Garfal, G.A. Navratil, H. Reimerdes, C lumbia U., M.S. Chu, G.L. Jacksn, T.H. Jensen, R.J. La Haye, J.T. Scville, E.J. Strait, G A, R.J. Jayakumar, LLNL, D.H. Edgell, FAR -T E C H, Inc "Active C ntrl f MHD S tability: E xtensin t the B urning P lasma R egime " University f Texas-Austin Nvember 3-5,2003
2 RWM Feedback System Has Been Imprved with New Hardware: :Newly-installed I-cils, New ff midplane Sensrs, SPA upgrade and PCS upgrade Cils being installed in DIII D New I-cil x New Sensrs Existing C-cil
3
4 Dynamic Errr Crrectin Prcess Maintains Identical Plasma Rtatin by use f Either C-Cil r I-Cil Ip betan/(2.4li) C-cil cur. (ka) I-cil cur (ka) Plasma Rtatin km/s) Full C-cil crrectin Full I-cil Crrectin
5 I-cil at Dynamic Resnant Errr field Crrectin is as Effective as C-Cils Maintaining High Plasma Rtatin
6 Dynamic Errr Field Crrectin with I-Cil Maintains Plasma Rtatin by Requesting Different Level f Current fr Different Cil Cnnectin I-cil current needed fr resnant errr field cmpensatin (amplitude: ka) cil current limit Disrupted with RWM time cnstant 0.0 Rtatin (km/s) DIII D N ATION AL FU S ION FAC ILITY Upper/Lwer I-cil cnnectin angle
7 I-cil Feedback Has Opened Higher bn Access Even If the Rtatin is Reduced during Discharge Imprved Time Respnse bserved in the Cntrl n ELM Induced RWM b / n.wall n b n sensr (G) db(g) ideal wall limit C b 1.0 Gp/Gd=40/20 q=2 MARS predictin Gp/Gd=40/80 Gp/Gd=40/0 Gp/Gd=40/40 I-cil Gp/Gd / / / / N FB D-alpha ªzer rtatin C-COIL: Gp/Gd=57/0 time rt (km/s) n wall limit 0.0 n feedback Rtatin (km/s) data with strng Ip ramp lw-q (q95ª3.0) 2.4li plasma DIII D N ATION AL FU S ION FAC ILITY C b = n.wall (b n - b ) n ( b ideal.wall n.wall - b ) n n
8 Dynamic Resnant Errr Field Crrectin Prcesss with Feedback High gain limit (K -> ) RESONANT AMPLIFICATION FACTOR <pl Apl K FEEDBACK GAIN Berrr> I_errr Bprepr> I_prepr } -initial guessing - Bfb> I_fb? Estimated Ttal Current fr Errr Cmpensatin = I_fb + I_prepr = -<pl Berrr> <pl Bfb> I_errr + I_prepr * e + 1/(K*Apl) [...] Better cupling between the feedback and plasma -> lwer crrectin current What is pssible cupling mechanism?
9 Pssible frmulatin fr cuplings : Trque in the tridal directin: Frce in tridal directin F = ( f d j pl x B ext ) f dj pl,n = s db pl. f.- (1/R) f db pl. q dj pl,q = f db pl.n.- (1/R) n db pl. f = - f [ db pl. q B ext.q + db pl. n. B ext.n ] Assumptin: - db pl. f. ª 0: Lcal Trque Integrated ver the surface: Ú F f R ds Vlume integrated trque Phase shift : negative feedback autmatically minimizes the shift
10 m=2 x r m=1 f m=3 m=5 m=4
11 dbn n : q= 2-, 2+,3, 4, 5
12 Mde Structure
13 Bn Field Pattern n q =3 Surface C-cil plidal directin I-cil Plasma mde 0.0 tridal directin (degrees) 360 * 0 degrees in the uter mid-plane
14 Lcal Trque Pattern n Surface: C-cil ( t= 2500 ms) I-cil (2600 ms) q= plidaldirectin q=3 tridal directin tridal directin
15 Nrmal and plidal field by C-cil Nrmal Field Plidal field C-cil Plasma B*B
16 Nrmal and plidal field by I-cil(240deg) Nrmal Field Plidal field I-cil Plasma B*B
17 Trque arund q=3 Surface by I-cil with Actual I-cil Current at t=2600ms Matches with Trque with C-cil by Actual cil current at 2500ms C-cil q=2(-) I-cil q=4 q=2(+) q=5 Full C-cil crrectin Full I-cil Crrectin q=3 Tridal angle relative t the Mde and applied field q=edge Tridal angle relative t the Mde and applied field
18 Trque by I-cil Matches with C-cil Trque arund qª 3 Surface Trque with I-cil with C-cil Df phase difference (degrees) edge Df : Phase Shift between Trque Estimated with C-cil curent at 2500 ms and I-cil current at 2600 ms and I-cil (degrees)
19 Dynamic Errr Field Crrectin with I-Cil Maintains Plasma Rtatin by Requesting Different Level f Current fr Different Cil Cnnectin I-cil current needed fr resnant errr field cmpensatin (amplitude: ka) cil current limit Disrupted with RWM time cnstant 0.0 Rtatin (km/s) DIII D N ATION AL FU S ION FAC ILITY Upper/Lwer I-cil cnnectin angle
20 Effective Averaged Field with Varius Upper / Lwer I-cil Cnnectin Can Be Estimated Using Surface Averaged Trque db eff q-edge q=5 q=4 q=3 q= Upper/Lwer I-cil cnnectin (degrees) Ú db ext db ds db = n.pl eff db ds n.pl Ú Current fr dynamic crrectin 1 /db eff
21 I-cil current needed fr resnant errr field cmpensatin (amplitude: ka) Resnant Errr Field Cmpensatin is Mst Effective when I-cil Field Cuples with RWM Structure at q=4 - I-cil pitch was scanned by varying upper/lwer I-cil cnnectin cil current limit Disrupted with RWM time cnstant Estimate with the cupling at q=4 0.0 Estimated I-cil cupling t RWM Bn (gauss/ka) 1.0 q-edge q=3 q=4 q= q= I-cil cnnectin angle 400 DIII D N ATION AL FU S ION FAC ILITY residual errr assumed at 45 deg.
22 I-cil Feedback Has Opened Higher bn Access Even If the Rtatin is Reduced during Discharge Imprved Time Respnse bserved in the Cntrl n ELM Induced RWM b / n.wall n b n sensr (G) db(g) ideal wall limit C b 1.0 Gp/Gd=40/20 q=2 MARS predictin Gp/Gd=40/80 Gp/Gd=40/0 Gp/Gd=40/40 I-cil Gp/Gd / / / / N FB D-alpha ªzer rtatin C-COIL: Gp/Gd=57/0 time rt (km/s) n wall limit 0.0 n feedback Rtatin (km/s) data with strng Ip ramp lw-q (q95ª3.0) 2.4li plasma DIII D N ATION AL FU S ION FAC ILITY C b = n.wall (b n - b ) n ( b ideal.wall n.wall - b ) n n
23 Direct Feedback is Observable n Feedback Respnse t ELM induced RFA_RWM Fast Respnse Cmpnent Amplitude Impact n after ELMs Feedback n A sensr signal (MPID067U) D-alpha 1200 time (ms) 1600 DIII D N ATION AL FU S ION FAC ILITY
24 Fast Respnse Cmpnent Amplitude Befre Feedback Feedback n ELMs A sensr signal (MPID067U) D-alpha 1250 time (ms) time (ms) 1350
25 Fast Respnse Cmpnent Amplitude Feedback n Feedback n A sensr signal (MPID067U) D-alpha 1300 time (ms) time (ms) 1450
26 Fast Respnse Cmpnent Amplitude Feedback n Feedback n A sensr signal (MPID067U) D-alpha 1450 time (ms) time (ms) 1550
27 Feedback with I-cil Imprved the Time Respnse up t wt ª 3 w C-Cil I-Cil N Feedback N Feedback Gp/Gd=57/57 FB n 1250 time(ms) time(ms) N feedback Gp/Gd=40/40 FB n db (G) C-cil I-cil freq(khz) /195/826/820.ai DIII D N ATION AL FU S ION FAC ILITY
28 SUMMARY Dynamic Resnant Errr Field Crrectin with C-COIl and I-COIL - Identical Impact n Plasma Rtatin - I-cil Cnnectin Flexibility -> Parametric Dependence Lcal Trque Hypthesis Prvides a Cnsistent Interpretatin I-Cil Imprved Time Respnse, better Cntrl n RFA& RWM
29 I-Cil feedback Imprved the Respnse arund wt = Stable RWM respnse t ELM induced n=1 perturbatin w H-alpha MPID averaged c-cil I-cil freq((khz) freq((khz) C-cil: Gp/Gd=57/ I-cil : Gp/Gd=40/ Next Issue: the cntrl at wt = 5-10 regime with feedback ptimizatin and further hardware imprvement w QQ/197/822/cmp/FFT.ai
30 Fast Respnse f Feedback is Taking Place with I_cil_FB ª 1 ka ( < 1gauss) 4.0 Gp/Gd= 40/40 40/0 40/20 Feedback Requested Current (ka) Cmmn fr varius gain setting Fast Feedback Fine Tuning by Dynamic Errr Field crrectin Ttal errr field Preprgrammed errr field crrectin phase / / / / time(ms) 1600 ffset-&angle-subtractin/#2.ai DIII D N ATION AL FU S ION FAC ILITY
31 Direct Feedback Cmpnent is ª 1kA ( 1 gauss n plasma) ms ms ms ms 1 ka 2 ka DIII D N ATION AL FU S ION FAC ILITY
DIII D. by M. Okabayashi. Presented at 20th IAEA Fusion Energy Conference Vilamoura, Portugal November 1st - 6th, 2004.
Control of the Resistive Wall Mode with Internal Coils in the Tokamak (EX/3-1Ra) Active Measurement of Resistive Wall Mode Stability in Rotating High Beta Plasmas (EX/3-1Rb) by M. Okabayashi Presented
More informationRWM FEEDBACK STABILIZATION IN DIII D: EXPERIMENT-THEORY COMPARISONS AND IMPLICATIONS FOR ITER
GA A24759 RWM FEEDBACK STABILIZATION IN DIII D: EXPERIMENT-THEORY COMPARISONS AND IMPLICATIONS FOR ITER by A.M. GAROFALO, J. BIALEK, M.S. CHANCE, M.S. CHU, D.H. EDGELL, G.L. JACKSON, T.H. JENSEN, R.J.
More informationExtended Lumped Parameter Model of Resistive Wall Mode and The Effective Self-Inductance
Extended Lumped Parameter Model of Resistive Wall Mode and The Effective Self-Inductance M.Okabayashi, M. Chance, M. Chu* and R. Hatcher A. Garofalo**, R. La Haye*, H. Remeirdes**, T. Scoville*, and T.
More informationResistive Wall Mode Control in DIII-D
Resistive Wall Mode Control in DIII-D by Andrea M. Garofalo 1 for G.L. Jackson 2, R.J. La Haye 2, M. Okabayashi 3, H. Reimerdes 1, E.J. Strait 2, R.J. Groebner 2, Y. In 4, M.J. Lanctot 1, G.A. Navratil
More informationRequirements for Active Resistive Wall Mode (RWM) Feedback Control
Requirements for Active Resistive Wall Mode (RWM) Feedback Control Yongkyoon In 1 In collaboration with M.S. Chu 2, G.L. Jackson 2, J.S. Kim 1, R.J. La Haye 2, Y.Q. Liu 3, L. Marrelli 4, M. Okabayashi
More informationMAGNETIC FIELD ERRORS: RECONCILING MEASUREMENT, MODELING AND EMPIRICAL CORRECTIONS ON DIII D
MAGNETIC FIELD ERRORS: RECONCILING MEASUREMENT, MODELING AND EMPIRICAL CORRECTIONS ON DIII D by M.J. Schaffer, T.E. Evans, J.L. Luxon, G.L. Jackson, J.A. Leuer, J.T. Scoville Paper QP1.76 Presented at
More informationRESISTIVE WALL MODE STABILIZATION RESEARCH ON DIII D STATUS AND RECENT RESULTS
RESISTIVE WALL MODE STABILIZATION RESEARCH ON STATUS AND RECENT RESULTS by A.M. Garofalo1 in collaboration with J. Bialek,1 M.S. Chance,2 M.S. Chu,3 T.H. Jensen,3 L.C. Johnson,2 R.J. La Haye,3 G.A. Navratil,1
More informationSTABILIZATION OF THE RESISTIVE WALL MODE IN DIII D BY PLASMA ROTATION AND MAGNETIC FEEDBACK
GA A24014 STABILIZATION OF THE RESISTIVE WALL MODE IN DIII D BY PLASMA ROTATION AND MAGNETIC FEEDBACK by M. Okabayashi, J. Bialek, M.S. Chance, M.S. Chu, E.D. Fredrickson, A.M. Garofalo, R. Hatcher, T.H.
More informationEffect of Resonant and Non-resonant Magnetic Braking on Error Field Tolerance in High Beta Plasmas
1 EX/5-3Ra Effect of Resonant and Non-resonant Magnetic Braking on Error Field Tolerance in High Beta Plasmas H. Reimerdes 1), A.M. Garofalo 2), E.J. Strait 2), R.J. Buttery 3), M.S. Chu 2), Y. In 4),
More informationGA A26242 COMPREHENSIVE CONTROL OF RESISTIVE WALL MODES IN DIII-D ADVANCED TOKAMAK PLASMAS
GA A26242 COMPREHENSIVE CONTROL OF RESISTIVE WALL MODES IN DIII-D ADVANCED TOKAMAK PLASMAS by M. OKABAYASHI, I.N. BOGATU, T. BOLZONELLA, M.S. CHANCE, M.S. CHU, A.M. GAROFALO, R. HATCHER, Y. IN, G.L. JACKSON,
More informationResistive Wall Mode Studies in a Reversed Field Pinch with Rotating Helical Field
J. Plasma FusirL Res. SERIES, Vl. 5 (22) 59-513 Resistive Wall Mde Studies in a Reversed Field Pinch with Rtating Helical Field MASAMUNE Sada and IIDA Mtmi Kyt Institute f Technlgy, Matsugasaki, Kyt 66-8585,
More informationEffects of Noise in Time Dependent RWM Feedback Simulations
Effects of Noise in Time Dependent RWM Feedback Simulations O. Katsuro-Hopkins, J. Bialek, G. Navratil (Department of Applied Physics and Applied Mathematics, Columbia University, New York, NY USA) Building
More informationGA A26247 EFFECT OF RESONANT AND NONRESONANT MAGNETIC BRAKING ON ERROR FIELD TOLERANCE IN HIGH BETA PLASMAS
GA A26247 EFFECT OF RESONANT AND NONRESONANT MAGNETIC BRAKING ON ERROR FIELD TOLERANCE IN HIGH BETA PLASMAS by H. REIMERDES, A.M. GAROFALO, E.J. STRAIT, R.J. BUTTERY, M.S. CHU, Y. In, G.L. JACKSON, R.J.
More informationOP AMP CHARACTERISTICS
O AM CHAACTESTCS Static p amp limitatins EFEENCE: Chapter 5 textbk (ESS) EOS CAUSED BY THE NUT BAS CUENT AND THE NUT OFFSET CUENT Op Amp t functin shuld have fr the input terminals a DC path thrugh which
More informationRWM Control in FIRE and ITER
RWM Control in FIRE and ITER Gerald A. Navratil with Jim Bialek, Allen Boozer & Oksana Katsuro-Hopkins MHD Mode Control Workshop University of Texas-Austin 3-5 November, 2003 OUTLINE REVIEW OF VALEN MODEL
More informationDynamical plasma response of resistive wall modes to changing external magnetic perturbations a
PHYSICS OF PLASMAS VOLUME 11, NUMBER 5 MAY 2004 Dynamical plasma response of resistive wall modes to changing external magnetic perturbations a M. Shilov, b) C. Cates, R. James, A. Klein, O. Katsuro-Hopkins,
More informationDynamical plasma response of resistive wall modes to changing external magnetic perturbations
Dynamical plasma response of resistive wall modes to changing external magnetic perturbations M. Shilov, C. Cates, R. James, A. Klein, O. Katsuro-Hopkins, Y. Liu, M. E. Mauel, D. A. Maurer, G. A. Navratil,
More informationCSA$-9 k067s-~ STUDY OF THE RESISTIVE WALL MODE IN DIII-D GAMA22921 JULY 1998
STUDY OF THE RESISTIVE WALL MODE IN DIIID GAMA22921 CSA$9 k067s~ by A.M. GAROFALO, J. BIALEK, M.S. CHU, E.D. FREDRICKSON, R.J. GROEBNER, R.J. La HAYE, L.L. LAO, G.A. NAVRATIL, B.W. RICE, S.A. SABBAGH,
More informationPrinceton Plasma Physics Laboratory. Multi-mode analysis of RWM feedback with the NMA Code
Princeton Plasma Physics Laboratory Multi-mode analysis of RWM feedback with the NMA Code M. S. Chance, M.Okabayashi, M. S. Chu 12 th Workshop on MHD Stability Control: Improved MHD Control Configurations
More informationGA A27444 PROBING RESISTIVE WALL MODE STABILITY USING OFF-AXIS NBI
GA A27444 PROBING RESISTIVE WALL MODE STABILITY USING OFF-AXIS NBI by J.M. HANSON, F. TURCO M.J. LANCTOT, J. BERKERY, I.T. CHAPMAN, R.J. LA HAYE, G.A. NAVRATIL, M. OKABAYASHI, H. REIMERDES, S.A. SABBAGH,
More informationOverview of Recent Experimental Results From the DIII D Advanced Tokamak Program
OV/-5 Overview of Recent Experimental Results From the DIII D Advanced Tokamak Program K.H. Burrell for the DIII D Team General Atomics, P.O. Box 8568, San Diego, California 986-568 email: burrell@fusion.gat.com
More informationOTHER USES OF THE ICRH COUPL ING CO IL. November 1975
OTHER USES OF THE ICRH COUPL ING CO IL J. C. Sprtt Nvember 1975 -I,," PLP 663 Plasma Studies University f Wiscnsin These PLP Reprts are infrmal and preliminary and as such may cntain errrs nt yet eliminated.
More informationModeling of resistive wall mode and its control in experiments and ITER a
Modeling of resistive wall mode and its control in experiments and ITER a Yueqiang Liu b Department of Applied Mechanics, EURATOM/VR Fusion Association, Chalmers University of Technology, Göteborg, Sweden
More informationPlasma Response Control Using Advanced Feedback Techniques
Plasma Response Control Using Advanced Feedback Techniques by M. Clement 1 with J. M. Hanson 1, J. Bialek 1 and G. A. Navratil 1 1 Columbia University Presented at 59 th Annual APS Meeting Division of
More informationResistive Wall Mode Stabilization and Plasma Rotation Damping Considerations for Maintaining High Beta Plasma Discharges in NSTX
1 EXS/5-5 Resistive Wall Mode Stabilization and Plasma Rotation Damping Considerations for Maintaining High Beta Plasma Discharges in NSTX S.A. Sabbagh 1), J.W. Berkery 1), J.M. Bialek 1), R.E. Bell ),
More informationThe Effects of Noise and Time Delay on RWM Feedback System Performance
The Effects of Noise and Time Delay on RWM Feedback System Performance O. Katsuro-Hopkins, J. Bialek, G. Navratil (Department of Applied Physics and Applied Mathematics, Columbia University, New York,
More informationThe general linear model and Statistical Parametric Mapping I: Introduction to the GLM
The general linear mdel and Statistical Parametric Mapping I: Intrductin t the GLM Alexa Mrcm and Stefan Kiebel, Rik Hensn, Andrew Hlmes & J-B J Pline Overview Intrductin Essential cncepts Mdelling Design
More informationNetworkable Fan Coil Controller
Netwrkable Fan Cil Cntrller EFCB-OE1 Series EFCB10T OE1 (24Vac / 0 relays) EFCB12T OE1 (240Vac / 0 relays) EFCB10TU4 OE1 (24Vac / 4 relays) EFCB12TU2 OE1 (240Vac / 2 relays) EFCB12TU4 OE1 (240Vac / 4 relays)
More informationResistive Wall Mode Observation and Control in ITER-Relevant Plasmas
Resistive Wall Mode Observation and Control in ITER-Relevant Plasmas J. P. Levesque April 12, 2011 1 Outline Basic Resistive Wall Mode (RWM) model RWM stability, neglecting kinetic effects Sufficient for
More informationGlobal Mode Control and Stabilization for Disruption Avoidance in High-β NSTX Plasmas *
1 EX/P8-07 Global Mode Control and Stabilization for Disruption Avoidance in High-β NSTX Plasmas * J.W. Berkery 1, S.A. Sabbagh 1, A. Balbaky 1, R.E. Bell 2, R. Betti 3, J.M. Bialek 1, A. Diallo 2, D.A.
More informationElectronic Fan Coil Controller
Electrnic Fan Cil Cntrller EFCB10TU2 EFCB10TU4 EFCB11TU2 EFCB11TU4 EFCB12TU2 EFCB12TU4 (24Vac / 2 relays) (24Vac / 4 relays) (120Vac / 2 relays) (120Vac /4 relays) (240Vac / 2 relays) (240Vac / 4 relays)
More informationResistive wall mode stabilization by slow plasma rotation in DIII-D tokamak discharges with balanced neutral beam injection a
PHYSICS OF PLASMAS 14, 056101 2007 Resistive wall mode stabilization by slow plasma rotation in DIII-D tokamak discharges with balanced neutral beam injection a E. J. Strait, b A. M. Garofalo, c G. L.
More informationRWM Control Code Maturity
RWM Control Code Maturity Yueqiang Liu EURATOM/CCFE Fusion Association Culham Science Centre Abingdon, Oxon OX14 3DB, UK Work partly funded by UK EPSRC and EURATOM. The views and opinions expressed do
More informationAPPLICATION GUIDE (v4.1)
2.2.3 VitalSensrs VS-300 Sensr Management Statin Remte/Relay Guide Implementing Remte-IN/Relay-OUT Digital I/O Fieldbus Objective: Equipment: Becme familiar with the instrument wiring requirements fr the
More informationPlasma Stability in Tokamaks and Stellarators
Plasma Stability in Tokamaks and Stellarators Gerald A. Navratil GCEP Fusion Energy Workshop Princeton, NJ 1- May 006 ACKNOWLEDGEMENTS Borrowed VGs from many colleagues: J. Bialek, A. Garofalo,R. Goldston,
More informationCourse Stabilty of Structures
Curse Stabilty f Structures Lecture ntes 2015.03.06 abut 3D beams, sme preliminaries (1:st rder thery) Trsin, 1:st rder thery 3D beams 2:nd rder thery Trsinal buckling Cupled buckling mdes, eamples Numerical
More informationAdvances in Global MHD Mode Stabilization Research on NSTX
1 EX/5-1 Advances in Global MHD Mode Stabilization Research on NSTX S.A. Sabbagh 1), J.W. Berkery 1), R.E. Bell 2), J.M. Bialek 1), S.P. Gerhardt 2), J.E. Menard 2), R. Betti 3), D.A. Gates 2), B. Hu 3),
More informationA water level indicator or other measuring device to determine the current depth to the water.
Fr Aqua4Plus 1.9.7 and later r Aqua4Plus Lite 2.1.1 r later. (Fr earlier versins r if using a PT2X with firmware lwer than 1.5, see Applicatin Nte 9C0152) Intrductin Purpse f this dcument is t prvide a
More information1999 RESEARCH SUMMARY
1999 RESEARCH SUMMARY by S.L. Allen Presented to DIII D Program Advisory Committee Meeting January 2 21, 2 DIII D NATIONAL FUSION FACILITY SAN DIEGO 3 /SLA/wj Overview of Physics Results from the 1999
More informationFormal Uncertainty Assessment in Aquarius Salinity Retrieval Algorithm
Frmal Uncertainty Assessment in Aquarius Salinity Retrieval Algrithm T. Meissner Aquarius Cal/Val Meeting Santa Rsa March 31/April 1, 2015 Outline 1. Backgrund/Philsphy 2. Develping an Algrithm fr Assessing
More informationD.J. Schlossberg, D.J. Battaglia, M.W. Bongard, R.J. Fonck, A.J. Redd. University of Wisconsin - Madison 1500 Engineering Drive Madison, WI 53706
D.J. Schlossberg, D.J. Battaglia, M.W. Bongard, R.J. Fonck, A.J. Redd University of Wisconsin - Madison 1500 Engineering Drive Madison, WI 53706 Non-solenoidal startup using point-source DC helicity injectors
More informationLevel Control in Horizontal Tank by Fuzzy-PID Cascade Controller
Wrld Academy f Science, Engineering and Technlgy 5 007 Level Cntrl in Hrizntal Tank by Fuzzy-PID Cascade Cntrller Satean Tunyasrirut, and Santi Wangnipparnt Abstract The paper describes the Fuzzy PID cascade
More informationA Self-Sensing Homopolar Magnetic Bearing: Analysis and Experimental Results
A Self-Sensing Hmplar Magnetic Bearing: Analysis and Experimental Results Perry Tsa Seth R. Sanders Gabriel Risk Department f Electrical Engineering and Cmputer Science University f Califrnia, Berkeley
More informationMeasurement and modeling of three-dimensional equilibria in DIII-D
Measurement and modeling of three-dimensional equilibria in DIII-D M. J. Lanctot, H. Reimerdes, A. M. Garofalo, M. S. Chu, J. M. Hanson et al. Citation: Phys. Plasmas 18, 056121 (2011); doi: 10.1063/1.3593009
More informationAnalysis and modelling of MHD instabilities in DIII-D plasmas for the ITER mission
Analysis and modelling of MHD instabilities in DIII-D plasmas for the ITER mission by F. Turco 1 with J.M. Hanson 1, A.D. Turnbull 2, G.A. Navratil 1, C. Paz-Soldan 2, F. Carpanese 3, C.C. Petty 2, T.C.
More informationDisruption dynamics in NSTX. long-pulse discharges. Presented by J.E. Menard, PPPL. for the NSTX Research Team
Disruption dynamics in NSTX long-pulse discharges Presented by J.E. Menard, PPPL for the NSTX Research Team Workshop on Active Control of MHD Stability: Extension of Performance Monday, November 18, 2002
More informationGENERAL FORMULAS FOR FLAT-TOPPED WAVEFORMS. J.e. Sprott. Plasma Studies. University of Wisconsin
GENERAL FORMULAS FOR FLAT-TOPPED WAVEFORMS J.e. Sprtt PLP 924 September 1984 Plasma Studies University f Wiscnsin These PLP Reprts are infrmal and preliminary and as such may cntain errrs nt yet eliminated.
More informationDIII D Research in Support of ITER
Research in Support of ITER by E.J. Strait and the Team Presented at 22nd IAEA Fusion Energy Conference Geneva, Switzerland October 13-18, 28 DIII-D Research Has Made Significant Contributions in the Design
More informationElectric Duct Heater. HECB Series Modbus Communication Module User Guide. HECB-Modbus Guide docx
Electric Duct Heater HECB Series Mdbus Cmmunicatin Mdule User Guide HECB-Mdbus Guide-150630.dcx Mdbus User Guide Cntents Intrductin... 1 Hlding s Table... 2 Table Glssary... 2 Hlding Table... 2 Ntes...
More informationKirchhoff Hypothesis. MER452: Composite Materials
Kirchhff Hpthesis MER45: Cmpsite Materials 1 Cmpsite Design Eperimental Data STRUCTURE CONSTITUENTS COMPOSITE Micr Mechanics STRUCTURAL ELEMENT ELEMENTARY STRUCTURE Finite Element Analsis E E G Classical
More informationMeasurement of Radial Loss and Lifetime. of Microwave Plasma in the Octupo1e. J. C. Sprott PLP 165. Plasma Studies. University of Wisconsin DEC 1967
Measurement f Radial Lss and Lifetime f Micrwave Plasma in the Octup1e J. C. Sprtt PLP 165 Plasma Studies University f Wiscnsin DEC 1967 1 The number f particles in the tridal ctuple was measured as a
More informationKSTAR Equilibrium Operating Space and Projected Stabilization at High Normalized Beta
1 THS/P2-05 KSTAR Equilibrium Operating Space and Projected Stabilization at High Normalized Beta Y.S. Park 1), S.A. Sabbagh 1), J.W. Berkery 1), J.M. Bialek 1), Y.M. Jeon 2), S.H. Hahn 2), N. Eidietis
More informationMetering Principles & Configurations
Metering Principles & Cnfiguratins CT PT Startc Western Energy Cmpany DCS Presenters Western Energy Cmpany Mnte Wilke Electrical Superintendent Curt Brckel Electrical Supervisr Brady Clbert Electrical
More informationNTC Thermistors, High Temperature Sensors
NTC Thermistrs, High Temperature Sensrs 2322 633 3/5/8... Vishay BCcmpnents FEATURES Small diameter Quick respnse t temperature change High stability ver a lng life Wide temperature range frm 4 t +2 C
More informationJ. C. Sprott OHMIC HEATING RATE IN A TOROIDAL OCTUPOLE. August 1975 PLP 643. Plasma Studies. University of Wisconsin
OHMC HEATNG RATE N A TORODAL OCTUPOLE J. C. Sprtt August 1975 PLP 643 Plasma Studies University f Wiscnsin These PLP Reprts are infrmal and preliminary and as such may cntain errrs nt yet eliminated. Tbey
More informationFIELD QUALITY IN ACCELERATOR MAGNETS
FIELD QUALITY IN ACCELERATOR MAGNETS S. Russenschuck CERN, 1211 Geneva 23, Switzerland Abstract The field quality in the supercnducting magnets is expressed in terms f the cefficients f the Furier series
More informationAttempts at Ion Cyclotron Heating. In a Toroidal Octupole. Presented at the Los Angeles Meeting of the American Physical Society. November 12-15, 1969
Attempts at n Cycltrn Heating n a Tridal Octuple by J. C. Sprtt Presented at the Ls Angeles Meeting f the American Physical Sciety Nvember 1215, 1969 PLP 321 These PLP Reprts are infnnal and preliminary
More informationLinearization of the Output of a Wheatstone Bridge for Single Active Sensor. Madhu Mohan N., Geetha T., Sankaran P. and Jagadeesh Kumar V.
Linearizatin f the Output f a Wheatstne Bridge fr Single Active Sensr Madhu Mhan N., Geetha T., Sankaran P. and Jagadeesh Kumar V. Dept. f Electrical Engineering, Indian Institute f Technlgy Madras, Chennai
More informationA New Resistive Response to 3-D Fields in Low Rotation H-modes
in Low Rotation H-modes by Richard Buttery 1 with Rob La Haye 1, Yueqiang Liu 2, Bob Pinsker 1, Jong-kyu Park 3, Holger Reimerdes 4, Ted Strait 1, and the DIII-D research team. 1 General Atomics, USA 2
More informationCHAPTER 8b Static Equilibrium Units
CHAPTER 8b Static Equilibrium Units The Cnditins fr Equilibrium Slving Statics Prblems Stability and Balance Elasticity; Stress and Strain The Cnditins fr Equilibrium An bject with frces acting n it, but
More informationEffect of an error field on the stability of the resistive wall mode
PHYSICS OF PLASMAS 14, 022505 2007 Effect of an error field on the stability of the resistive wall mode Richard Fitzpatrick Institute for Fusion Studies, Department of Physics, University of Texas at Austin,
More informationModule 4: General Formulation of Electric Circuit Theory
Mdule 4: General Frmulatin f Electric Circuit Thery 4. General Frmulatin f Electric Circuit Thery All electrmagnetic phenmena are described at a fundamental level by Maxwell's equatins and the assciated
More informationGASES. PV = nrt N 2 CH 4 CO 2 O 2 HCN N 2 O NO 2. Pressure & Boyle s Law Temperature & Charles s Law Avogadro s Law IDEAL GAS LAW
GASES Pressure & Byle s Law Temperature & Charles s Law Avgadr s Law IDEAL GAS LAW PV = nrt N 2 CH 4 CO 2 O 2 HCN N 2 O NO 2 Earth s atmsphere: 78% N 2 21% O 2 sme Ar, CO 2 Sme Cmmn Gasses Frmula Name
More informationPhysics 2B Chapter 23 Notes - Faraday s Law & Inductors Spring 2018
Michael Faraday lived in the Lndn area frm 1791 t 1867. He was 29 years ld when Hand Oersted, in 1820, accidentally discvered that electric current creates magnetic field. Thrugh empirical bservatin and
More informationDIII D INTEGRATED PLASMA CONTROL SOLUTIONS FOR ITER AND NEXT- GENERATION TOKAMAKS
GA A25808 DIII D INTEGRATED PLASMA CONTROL SOLUTIONS FOR ITER AND NEXT- GENERATION TOKAMAKS by D.A. HUMPHREYS, J.R. FERRON, A.W. HYATT, R.J. La HAYE, J.A. LEUER, B.G. PENAFLOR, M.L. WALKER, A.S. WELANDER,
More informationThree Dimensional Effects in Tokamaks How Tokamaks Can Benefit From Stellarator Research
1 TH/P9-10 Three Dimensional Effects in Tokamaks How Tokamaks Can Benefit From Stellarator Research S. Günter, M. Garcia-Munoz, K. Lackner, Ph. Lauber, P. Merkel, M. Sempf, E. Strumberger, D. Tekle and
More informationTHE DIII D PROGRAM THREE-YEAR PLAN
THE PROGRAM THREE-YEAR PLAN by T.S. Taylor Presented to Program Advisory Committee Meeting January 2 21, 2 3 /TST/wj PURPOSE OF TALK Show that the program plan is appropriate to meet the goals and is well-aligned
More informationProgress Toward High Performance Steady-State Operation in DIII D
Progress Toward High Performance Steady-State Operation in DIII D by C.M. Greenfield 1 for M. Murakami, 2 A.M. Garofalo, 3 J.R. Ferron, 1 T.C. Luce, 1 M.R. Wade, 1 E.J. Doyle, 4 T.A. Casper, 5 R.J. Jayakumar,
More informationDIII D. by F. Turco 1. New York, January 23 rd, 2015
Modelling and Experimenting with ITER: the MHD Challenge by F. Turco 1 with J.M. Hanson 1, A.D. Turnbull 2, G.A. Navratil 1, F. Carpanese 3, C. Paz-Soldan 2, C.C. Petty 2, T.C. Luce 2, W.M. Solomon 4,
More informationChallenges in advanced imaging with radio interferometric telescopes. S.Bhatnagar NRAO, Socorro April 08, 2005
Challenges in advanced imaging with radi interfermetric telescpes S.Bhatnagar NRAO, Scrr April 08, 2005 Basic Interfermetry Terminlgy: Visibility: V=, Ei is the electric field Baseline: Length f
More information2/3 Axis Position Indicator
SERIES Z-89 2/3 Axis Psitin Indicatr Pwer dwn memry Selectable decimal pint Multi edge functin Pulse factr Reference value External reset r preset inputs Digital brightness cntrl Z89-000-E_21-06.dc Dku
More informationELECTROSTATIC FIELDS IN MATERIAL MEDIA
MF LCTROSTATIC FILDS IN MATRIAL MDIA 3/4/07 LCTURS Materials media may be classified in terms f their cnductivity σ (S/m) as: Cnductrs The cnductivity usually depends n temperature and frequency A material
More informationLecture 24: Flory-Huggins Theory
Lecture 24: 12.07.05 Flry-Huggins Thery Tday: LAST TIME...2 Lattice Mdels f Slutins...2 ENTROPY OF MIXING IN THE FLORY-HUGGINS MODEL...3 CONFIGURATIONS OF A SINGLE CHAIN...3 COUNTING CONFIGURATIONS FOR
More information제어이론복습 강의보조자료. 박상혁
제어이론복습 강의보조자료 박상혁 ark@kau.ac.kr u inut t t utut : y t t u Linear System with zer C Linear System with zer C Linear System with zer C N k utut g t d g t : utut by imulse inut u gt u k g t k u g nvlutin
More informationFeasibility Testing Report Muscle Optimization Stage I
Feasibility Testing Reprt Muscle Optimizatin Stage I Team: P15001: Active Ankle Ft Orthtic Engineer: Nah Schadt Mechanical Engineer Engineer: Tyler Leichtenberger Mechanical Engineer Test Date: 10/14/2014
More informationFINITE ELEMENT CENTER
FINITE ELEMENT CENTER PREPRINT 25 7 Modeling of resistive wall mode and its control in experiments and ITER Yueqiang Liu, M.S. Chu, A.M. Garofalo, Y. Gribov, M. Gryaznevich, T.C. Hender, D.F. Howell, R.J.
More informationNon-Solenoidal Plasma Startup in
Non-Solenoidal Plasma Startup in the A.C. Sontag for the Pegasus Research Team A.C. Sontag, 5th APS-DPP, Nov. 2, 28 1 Point-Source DC Helicity Injection Provides Viable Non-Solenoidal Startup Technique
More informationName: Block: Date: Science 10: The Great Geyser Experiment A controlled experiment
Science 10: The Great Geyser Experiment A cntrlled experiment Yu will prduce a GEYSER by drpping Ments int a bttle f diet pp Sme questins t think abut are: What are yu ging t test? What are yu ging t measure?
More informationPerfrmance f Sensitizing Rules n Shewhart Cntrl Charts with Autcrrelated Data Key Wrds: Autregressive, Mving Average, Runs Tests, Shewhart Cntrl Chart
Perfrmance f Sensitizing Rules n Shewhart Cntrl Charts with Autcrrelated Data Sandy D. Balkin Dennis K. J. Lin y Pennsylvania State University, University Park, PA 16802 Sandy Balkin is a graduate student
More informationMechatronic Design of Hard Disk Drives: single and dual stage
K.N. Tsi University f Technlgy Advanced Rbtics and Autmated Systems Mechatrnic Design f Hard Disk Drives: single and dual stage Dr. Hamid D. Taghirad Advanced Rbtics and Autmated Systems (ARAS) Department
More informationMicro and Smart Systems
Micr and Smart Systems Lecture 33 OpAmps Circuits and signal cnditining fr micrsystems devices Prf K.N.Bhat, ECE Department, IISc Bangalre email: knbhat@gmail.cm Tpics fr Discussin Amplifiers and Op Amp
More informationResponse of a Resistive and Rotating Tokamak to External Magnetic Perturbations Below the Alfven Frequency
Response of a Resistive and Rotating Tokamak to External Magnetic Perturbations Below the Alfven Freuency by M.S. Chu In collaboration with L.L. Lao, M.J. Schaffer, T.E. Evans E.J. Strait (General Atomics)
More informationA Study on Pullout Strength of Cast-in-place Anchor bolt in Concrete under High Temperature
Transactins f the 7 th Internatinal Cnference n Structural Mechanics in Reactr Technlgy (SMiRT 7) Prague, Czech Republic, August 7 22, 23 Paper #H-2 A Study n Pullut Strength f Cast-in-place Anchr blt
More informationELM Suppression in DIII-D Hybrid Plasmas Using n=3 Resonant Magnetic Perturbations
1 EXC/P5-02 ELM Suppression in DIII-D Hybrid Plasmas Using n=3 Resonant Magnetic Perturbations B. Hudson 1, T.E. Evans 2, T.H. Osborne 2, C.C. Petty 2, and P.B. Snyder 2 1 Oak Ridge Institute for Science
More informationEarly detection of mining truck failure by modelling its operation with neural networks classification algorithms
RU, Rand GOLOSINSKI, T.S. Early detectin f mining truck failure by mdelling its peratin with neural netwrks classificatin algrithms. Applicatin f Cmputers and Operatins Research ill the Minerals Industries,
More informationNIMROD FROM THE CUSTOMER S PERSPECTIVE MING CHU. General Atomics. Nimrod Project Review Meeting July 21 22, 1997
NIMROD FROM THE CUSTOMER S PERSPECTIVE MING CHU General Atomics Nimrod Project Review Meeting July 21 22, 1997 Work supported by the U.S. Department of Energy under Grant DE-FG03-95ER54309 and Contract
More informationInteraction of scrape-off layer currents with magnetohydrodynamical instabilities in tokamak plasmas
Interaction of scrape-off layer currents with magnetohydrodynamical instabilities in tokamak plasmas Richard Fitzpatrick Institute for Fusion Studies Department of Physics University of Texas at Austin
More informationGeneral Chemistry II, Unit I: Study Guide (part I)
1 General Chemistry II, Unit I: Study Guide (part I) CDS Chapter 14: Physical Prperties f Gases Observatin 1: Pressure- Vlume Measurements n Gases The spring f air is measured as pressure, defined as the
More informationGuaranteeing Reliability with Vibration Simulation and Testing. Dr. Nathan Blattau
Guaranteeing Reliability with Vibratin Simulatin and Testing Dr. Nathan Blattau . Nathan Blattau, Ph.D. - Senir Vice President Has been invlved in the packaging and reliability f electrnic equipment fr
More information1. Transformer A transformer is used to obtain the approximate output voltage of the power supply. The output of the transformer is still AC.
PHYSIS 536 Experiment 4: D Pwer Supply I. Intrductin The prcess f changing A t D is investigated in this experiment. An integrated circuit regulatr makes it easy t cnstruct a high-perfrmance vltage surce
More informationGA A23430 ADVANCED TOKAMAK PHYSICS IN DIII D
GA A343 ADVANCED TOKAMAK PHYSICS IN DIII D by C.C. PETTY, T.C. LUCE, P.A. POLITZER, M.R. WADE, S.L. ALLEN, M.E. AUSTIN, B. BRAY, K.H. BURRELL, T.A. CASPER, M.S. CHU, J.R. FERRON, E.D. FREDRICKSON, A.M.
More informationPSU GISPOPSCI June 2011 Ordinary Least Squares & Spatial Linear Regression in GeoDa
There are tw parts t this lab. The first is intended t demnstrate hw t request and interpret the spatial diagnstics f a standard OLS regressin mdel using GeDa. The diagnstics prvide infrmatin abut the
More informationAir distribution systems. Please note, type code is new, see last page. Floor twist outlets DB-E... for commercial rooms DS 1146 E 02.
Air distributin systems Please nte, type cde is new, see last page. Flr twist utlets DB-E... fr cmmercial rms DS E 0.0/ Flr twist utlets nstructin design Preliminary remarks Air utlets frm KRANTZ KOMPONENTEN
More informationSMART TESTING BOMBARDIER THOUGHTS
Bmbardier Inc. u ses filiales. Tus drits réservés. BOMBARDIER THOUGHTS FAA Bmbardier Wrkshp Mntreal 15-18 th September 2015 Bmbardier Inc. u ses filiales. Tus drits réservés. LEVERAGING ANALYSIS METHODS
More informationUniversal Pump Control
Universal Pump Cntrl Operatinal Instructins versin 1.00 UPC Operatinal Features The TXAM Pumps Universal Pump Cntrl is available in AC, DC r Brushless Mtr cnfiguratins. Can be cnfigured t perate ALL TXAM
More informationCOMP9444 Neural Networks and Deep Learning 3. Backpropagation
COMP9444 Neural Netwrks and Deep Learning 3. Backprpagatin Tetbk, Sectins 4.3, 5.2, 6.5.2 COMP9444 17s2 Backprpagatin 1 Outline Supervised Learning Ockham s Razr (5.2) Multi-Layer Netwrks Gradient Descent
More informationDataflow Analysis and Abstract Interpretation
Dataflw Analysis and Abstract Interpretatin Cmputer Science and Artificial Intelligence Labratry MIT Nvember 9, 2015 Recap Last time we develped frm first principles an algrithm t derive invariants. Key
More informationLeast Squares Optimal Filtering with Multirate Observations
Prc. 36th Asilmar Cnf. n Signals, Systems, and Cmputers, Pacific Grve, CA, Nvember 2002 Least Squares Optimal Filtering with Multirate Observatins Charles W. herrien and Anthny H. Hawes Department f Electrical
More informationNon-inductive plasma startup and current profile modification in Pegasus spherical torus discharges
Non-inductive plasma startup and current profile modification in Pegasus spherical torus discharges Aaron J. Redd for the Pegasus Team 2008 Innovative Confinement Concepts Workshop Reno, Nevada June 24-27,
More informationHypothesis Tests for One Population Mean
Hypthesis Tests fr One Ppulatin Mean Chapter 9 Ala Abdelbaki Objective Objective: T estimate the value f ne ppulatin mean Inferential statistics using statistics in rder t estimate parameters We will be
More information