EU Plasma-Wall Interactions Task Force
|
|
- Alvin Waters
- 5 years ago
- Views:
Transcription
1 Recent results on material migration and fuel retention in JET V. Philipps and JET TFE co-workers* Overview on present results on erosion, deposition and fuel retention in last JET campaign ( ,C5-C15) Recent results from QMB on local material transport Conclusions * P. Coad, A. Widdeshoven (UKAEA), J. Likonen (Tekes), M. Rubel (VR), M. Mayer (IPP), H.G. Esser, A. Kreter (FZJ)
2 Large effort to analyse erosion, material migration and fuel retention MK SRP campaign Divertor plasma sec(23 h) Louver clips Deposition monitor QMB Louver clips Deposition monitor 3 μm W stripe on poloidal row of divertor tiles Analysis by NRA, Sims, metallography on cross sections, T-off gas measurements
3 Long term samples in main chamber graphite plug probes on inner wall coated with 50 nm W layer or 280 nm Ni layer (exposed all times) M. Mayer et al, IPP Samples with thin layers of Be, C, Ni and W on different substrates behind flaps in octants 3 and 5, opened only during plasma discharges (4 samples behind and one outside)
4 No deposition EU Plasma-Wall Interactions Task Force Integral deposition in μm Deposit 3µm W W CFC erosion W JG c 100μm 50 μm 280μm 200μm No W layer Only 50% of time in C 14-C15 3µm W
5 73g Estimate : integrated deposition Total deposition inner and outer : 950 g ( C/sec) 63g 55g 35g 38 g 5g Total deposition inner: 543 g 35g louver 578 g total No clear erosion or deposition Outer 380g erosion 300g Louver: 35 g (from QMB) Not analysed yet Total deposition outer : 380 g
6 200 g on plasma viewing sides, majority ( 750g) on shadowed areas of base tiles 4 and 6 some part leaves towards louvers (estimate from QMB 35 g, needs additional input from deposition monitors) basic operating temperature : 80C (morning) - 140C(evening), but tile 1,3 much hotter during plasma operation Total C deposition : Only inner divertor: C/sec C/sec
7 Estimate: deuterium retention in layers D/C fraction tile 1,3: 0.2 D/C fraction tile 4 (and 6) g D D/ sec (of divertorplasma) [ Total D inlet : 1800g Relative fuel retention : 3.8 % ] No size scaling, ITER behaves like JET (50/50 D:T) mix 1x10 23 T/shot = 0.25gT/shot 1400 shot until limit Surface area(m 2 ) Power (MW) Particle flux (divertor) JET (avarage) ~ ITER 1000 (X 4 ) 350 (X 70) (x 400 ) A carbon ITER has large T inventory problems
8 D-Fluence RBS: Amount of W [10 18 Atoms/cm 2 ] x x x RBS PIXE 5 6 Outer vertical tile: net erosion 7 8 Before After Manipulator x [mm] Initial PIXE: Amount of W [a.u.] Dtile7 RBS analysis of W stripe before and after operation Erosion Remaining W Tile Distance (Z direction) cm erosion, large areas of complete W Non uniform W-erosion, W large areas of complete W-erosion M. Mayer, PSI 17
9 Main wall probes W layer erosion All main wall probes ( in between poloidal limiters) show erosion, 60 nm of W, all Ni layers (280 nm) totally eroded (W erosion behind and before flap about the same ) Erosion by charge exchange, modelling underway Main wall erosion dominated
10 Comparison of integrated material deposition 12 Only inner B Carbon Deposition ( / sec) Outer + inner AUG C dominated Recent results in AUG show a significant decrease under full W first wall conditions!! (M. Mayer et al) 0 JETMKIIA JETSRP JETMKGB DIII-D TEXTOR Similar material deposition rates in different carbon dominated devices
11 frequency [Hz] ISP at horizontal tile integral erosion 1 3 #64980 #64976 LBSRP QMB4 4 6 Recent QMB data from MK LBSRP campaign #65281 #65282 LBSRP QMB JET pulse # Integral deposition when inner strike point at vertical tile 3 Integral erosion when inner strike point at horizontal tile 4 PFR areas can turn form deposition to erosion dominated areas ISP at vertical tile integral deposition ISP at horizontal tile integral erosion 1 3 #65409 # LBSRP QMB4 ISP at vertical tile integral deposition A. Kreter, H. Esser #65667 #65668 ISP at horizontal tile integral erosion LBSRP QMB
12 7000 QMB1 (inner) and QMB5 (outer) data overview frequency [Hz] integral behaviour QMB1 (inner) QMB5 (outer) JET pulse # Integral deposition on inner and outer QMB louver outer louver deposition dominated but about a factor of 2.5 less compared with inner divertor
13 Material transport ways EU Plasma-Wall Interactions Task Force Under same strike point and plasma conditions, very reproducible deposition With plasma on tile 4, about 5 times more deposition in shots with larger Elms ( type I) than in L mode Dedicated Shot series have been performed on step wise C- transport, history effect First C deposition on vertical tiles In L mode or with small Elms small transport to tile 4 (also confirmed by 13 C deposition, L mode from top) Large transport to tile 4 with larger Elms (type I Elms) Large C transport to louver ( QMB) with plasma lying on tile 4 Transport much more effective with larger Elms then without In L mode or small Elms plasmas, majority of deposit would remain on tile 1,3
14 In agreement with all other observations, large net material deposition in inner divertor. In last campaign, 25% on plasma viewing sides, 75% on shadowed areas on base tiles, smaller amount leaves to louvers. Outer base tile also net deposition area also outer louver region but about 2.5 smaller deposition than on inner louver Total C deposition in divertor ( inner+outer ) from post mortem: C/sec, D retention estimation: D/sec Outer vertical strike point tile (7) erosion dominated Main chamber net erosion area Local divertor C transport ways determined by strike point and tile geometry. Local transport largely promoted by larger Elms PFR can change from deposition to erosion zone
15 Reserve slides
16 QMB currently in JET EU Plasma-Wall Interactions Task Force QMB # Features Position Shutter Working period QMB1 replacement system inner divertor, module 13 QMB2 heated inner divertor, module 02 yes QMB4 compact under LBSRP, module 02 no QMB5 heated outer divertor, module 02 yes monitoring Be QMB6 apron outer divertor, module 02 no evaporations yes now (68200) cabling problems during installation , then overheated (electronic failure in fast stop ) now (68200) 1 8 QMB 1,2,3 3 LBSRP 7 QMB 5 QMB 6 QMB 4 4 6
17 Deposit Deposit Deposit CFC bulk tile3 tile1 CFC bulk W stripe W stripe CFC bulk tile4 New data from recent JET campaign: inner divertor is always a deposition dominated region (P. Coad, J. Likonen, M. Roedig) V.Philipps, Seminar IPP, 30_03_06
18 CONCENTRATION RATIO: BERYLLIUM - TO - CARBON Be / C Inner M. Rubel et al Outer MKIIA DIVERTOR TILE (POLOIDAL DIRECTION) Present conditions Plasma facing sides: stable Be-C C mix (~Be( 2 C?) D content : Shadowed areas: more pure C layers D content: We need for more information on chemical state of deposits & influence of oxygen V.Philipps, Seminar IPP, 30_03_06
19 10C 1Be Present conditions Further C- transport by carbon chemistry (?) ~ Be 2 C (?) C layer C 1C(?) 10 Be New conditions (?)?? Further transport of Be (new PISCES data (?)) Be 2 W?? W C V.Philipps, Seminar IPP, 30_03_06
20 1. Understanding of in vessel T retention Example (1) After the JET DT1 T-experiment, 3.5 g of T (94%) was found in flakes, 0.1 g T (3%) was trapped by the 480 CFC divertor tiles (based on 100 analysis points) and 0.1 gt (3%) estimated to be trapped by the rest of the wall (N. Bekris, FZK ) From the T retained in the 480 CFC tiles, a significant fraction (20-50% typically) was found in depths larger then 1mm For fine grain graphite, the bulk retention fraction is much lower (about 1%) V. Philipps, IEA Greifswald 2006
21 Fuel retention in JET MkIIGB Divertor time: sec (16 hours) D injection: 766g Inner ion flux: 1.3x10 27 C deposition: 400g Rate: 3.4x10 20 Cs -1 Inner Divertor: D/C~0.2 Retention of 3% (25g) (MKII GB) D/C J Likonen, P Coad et al., (NRA: D/C ratio, SIMS: layer thicknesses) Only plasma facing surfaces at divertor included (not tile gaps, inner limiters...) -D retention in the divertor: 3% (Mk-IIGB), 2.4% (MKII-SRP).
22 AUG: 2002/2003: Deposition of D and C 8 6A 6B 5 4 9C M Mayer et al., PSI 2004 Deposition [10 19 at./cm 2 ] B + C D measured D assumed 2002/2003 campaign: Mainly carbon machine (45% W) Retention governed by trapping on inner tile surface (70% inner divertor tiles, 20% in remote ares (below roof baffle,...) Total retention ~4% of input (10-20% from gas balance) 2004/2005 campaign: Full W machine except the divertor (Carbon) No significant difference in retention between 2002/2003 and 2004/2005
23 layer D, at.% Be, at.% 12 C, at.% O, at.% Cr, at.% Poster Likonen
1 EX/3-5. Material Erosion and Redeposition during the JET MkIIGB-SRP Divertor Campaign
1 Material Erosion and Redeposition during the JET MkIIGB-SRP Divertor Campaign A. Kirschner 1), V. Philipps 1), M. Balden 2), X. Bonnin 3), S. Brezinsek 1), J.P. Coad 4), D. Coster 2), S.K. Erents 4),
More informationANALYSIS OF PLASMA FACING MATERIALS IN CONTROLLED FUSION DEVICES. Marek Rubel
ANALYSIS OF PLASMA FACING MATERIALS IN CONTROLLED FUSION DEVICES Marek Rubel Alfvén Laboratory, Royal Institute of Technology, Association EURATOM VR, Stockholm, Sweden Acknowledgements Paul Coad and Guy
More informationCarbon Deposition and Deuterium Inventory in ASDEX Upgrade
1 IAEA-CN-116 / EX / 5-24 Carbon Deposition and Deuterium Inventory in ASDEX Upgrade M. Mayer 1, V. Rohde 1, J. Likonen 2, E. Vainonen-Ahlgren 2, J. Chen 1, X. Gong 1, K. Krieger 1, ASDEX Upgrade Team
More informationERO modelling of local deposition of injected 13 C tracer at the outer divertor of JET
ERO modelling of local deposition of injected 13 C tracer at the outer divertor of JET M I Airila 1, L K Aho-Mantila 2, S Brezinsek 3, J P Coad 4, A Kirschner 3, J Likonen 1, D Matveev 3, M Rubel 5, J
More information1 EX/P4-8. Hydrogen Concentration of Co-deposited Carbon Films Produced in the Vicinity of Local Island Divertor in Large Helical Device
1 EX/P4-8 Hydrogen Concentration of Co-deposited Carbon Films Produced in the Vicinity of Local Island Divertor in Large Helical Device T. Hino 1,2), T. Hirata 1), N. Ashikawa 2), S. Masuzaki 2), Y. Yamauchi
More informationHydrocarbon transport in the MkIIa divertor of JET
INSTITUTE OF PHYSICS PUBLISHING Plasma Phys. Control. Fusion 45 (23) 39 319 PLASMA PHYSICS AND CONTROLLED FUSION PII: S741-3335(3)37188-X Hydrocarbon transport in the MkIIa divertor of JET A Kirschner
More informationIn-vessel Tritium Inventory in ITER Evaluated by Deuterium Retention of Carbon Dust
FT/P1-19 In-vessel Tritium Inventory in ITER Evaluated by Deuterium Retention of Carbon Dust T. Hino 1), H. Yoshida 1), M. Akiba 2), S. Suzuki 2), Y. Hirohata 1) and Y. Yamauchi 1) 1) Laboratory of Plasma
More informationGlobal migration of impurities in tokamaks: what have we learnt?
Global migration of impurities in tokamaks: what have we learnt? Euratom-Tekes Annual Seminar Silja Serenade, 28 May, 2013 Antti Hakola, Markus Airila and many others VTT Technical Research Centre of Finland
More informationITER A/M/PMI Data Requirements and Management Strategy
ITER A/M/PMI Data Requirements and Management Strategy Steven Lisgo, R. Barnsley, D. Campbell, A. Kukushkin, M. Hosokawa, R. A. Pitts, M. Shimada, J. Snipes, A. Winter ITER Organisation with contributions
More informationGlobal Erosion and Deposition Patterns in JET with the ITER-like Wall
CCFE-PR(15)25 A.Baron-Wiechec, A.Widdowson, E.Alves, C.F.Ayres, N. P. Barradas, S.Brezinsek, J.P.Coad, N.Catarino, K.Heinola, J.Likonen, G.F.Matthews, M.Mayer, P. Petersson, M.Rubel, W. van Renterghem,
More informationAssessment of Erosion, deposition and fuel retention in the JET-ILW divertor from Ion Beam Analysis data
EUROFUSION WPJET2-PR(16) 14813 N Catarino et al. Assessment of Erosion, deposition and fuel retention in the JET-ILW divertor from Ion Beam Analysis data Preprint of Paper to be submitted for publication
More informationEstimation of the contribution of gaps to tritium retention in the divertor of ITER
Estimation of contribution of gaps to tritium retention in the divertor of ITER 1 Estimation of the contribution of gaps to tritium retention in the divertor of ITER 1. Introduction D. Matveev 1,2, A.
More informationPower Deposition Measurements in Deuterium and Helium Discharges in JET MKIIGB Divertor by IR-Thermography
EFDA JET CP(02)01/03 T Eich, A Herrmann, P Andrew and A Loarte Power Deposition Measurements in Deuterium and Helium Discharges in JET MKIIGB Divertor by IR-Thermography . Power Deposition Measurements
More informationDeuterium and Hydrogen Retention Properties of the JT-60 and JT-60U Divertor Tiles
Deuterium and Hydrogen Retention Properties of the JT-60 and JT-60U Divertor Tiles Y. Hirohata 1), T. Tanabe 2), Y. Oya 3), K. Shibahara 4), M. Oyaidzu 5), T. Arai 6), K. Masaki 6), Y. Gotoh 6), K. Okuno
More informationChemical Erosion and Critical Issues for ITER
Chemical Erosion and Critical Issues for ITER J. Roth Max-Planck-Institut für Plasmaphysik, Garching Chemical Erosion Studies Erosion yields: Dependence on temperature, energy and flux Emitted hydrocarbons
More informationMicroanalysis of deposited layers in the divertor of JET with ITER-like wall
EUROFUSION WPJET2-PR(16) 14834 Y Zhou et al. Microanalysis of deposited layers in the divertor of JET with ITER-like wall Preprint of Paper to be submitted for publication in 22nd International Conference
More informationModelling of Carbon Erosion and Deposition in the Divertor of JET
EFDA JET CP(01)02-64 A. Kirschner, V. Philipps, P. Wienhold, W. Fundamenski, G. Matthews, P. Coad, M. Stamp, D. Coster, D. Elder, P. Stangeby and JET EFDA Contributors Modelling of Carbon Erosion and Deposition
More informationHelium effects on Tungsten surface morphology and Deuterium retention
1 Helium effects on Tungsten surface morphology and Deuterium retention Y. Ueda, H.Y. Peng, H. T. Lee (Osaka University) N. Ohno, S. Kajita (Nagoya University) N. Yoshida (Kyushu University) R. Doerner
More informationDeposition and re-erosion studies by means of local impurity injection in TEXTOR
Deposition and re-erosion studies by means of local impurity injection in TEXTOR A. Kirschner a*, A. Kreter a, P. Wienhold a, S. Brezinsek a, J.W. Coenen a, H.G. Esser a, A. Pospieszczyk a, Ch. Schulz
More informationDeuterium Inventory in Tore Supra: status of post mortem analyses
Deuterium Inventory in Tore Supra: status of post mortem analyses T. Dittmar a,*, P. Roubin d, E. Tsitrone a, E. Gauthier a, A. Hakola c, J. Likonen c, F. Linez a, C. Martin d, M. Mayer b, C. Pardanaud
More informationErosion of tungsten and carbon markers in the outer divertor of ASDEX Upgrade
Article published in Physica Scripta T128 (2007) 106 Erosion of tungsten and carbon markers in the outer divertor of ASDEX Upgrade M Mayer 1, V Rohde 1, G Ramos 2, E Vainonen-Ahlgren 3, J Likonen 3, J
More informationGlobal migration of impurities in tokamaks
Global migration of impurities in tokamaks A Hakola 1, M I Airila 1, C Björkas 2, D Borodin 3, S Brezinsek 3, J P Coad 1, M Groth 4, A Järvinen 4, A Kirschner 3, S Koivuranta 1, K Krieger 5, T Kurki-Suonio
More informationReview of experimental observations of plasma detachment and of the effects of divertor geometry on divertor performance
Review of experimental observations of plasma detachment and of the effects of divertor geometry on divertor performance Alberto Loarte European Fusion Development Agreement Close Support Unit - Garching
More informationLH Generated Hot Spots on the JET Divertor
LH Generated Hot Spots on the JET Divertor K.M. Rantamäki 1, V. Petržílka 2, F. Žáček 2, A. Ekedahl 3, K. Erents 4, V. Fuchs 2, M. Goniche 3, G. Granucci 5, S.J. Karttunen 1, J. Mailloux 4, and M.-L.Mayoral
More informationIon beam analysis methods in the studies of plasma facing materials in controlled fusion devices
Vacuum 70 (2003) 423 428 Ion beam analysis methods in the studies of plasma facing materials in controlled fusion devices M. Rubel a, *, P. Wienhold b, D. Hildebrandt c a Alfv!en Laboratory, Royal Institute
More informationComparison of tungsten fuzz growth in Alcator C-Mod and linear plasma devices
Comparison of tungsten fuzz growth in Alcator C-Mod and linear plasma devices G.M. Wright 1, D. Brunner 1, M.J. Baldwin 2, K. Bystrov 3, R. Doerner 2, B. LaBombard 1, B. Lipschultz 1, G. de Temmerman 3,
More informationDust Studies in Fusion Devices
Dust Studies in Fusion Devices D.L. Rudakov Presented at the PFC Meeting Boston MA July 7-10, 2009 10 µm Including contributions from A. Litnovsky, N. Asakura, N. Ashikawa, G. DeTemmerman, S. Ratynskaia
More informationThomas Schwarz-Selinger. Max-Planck-Institut for Plasmaphysics, Garching Material Science Division Reactive Plasma Processes
Max-Planck-Institut für Plasmaphysik Thomas Schwarz-Selinger Max-Planck-Institut for Plasmaphysics, Garching Material Science Division Reactive Plasma Processes personal research interests / latest work
More informationEffect of the Surface Temperature on Net Carbon Deposition and Deuterium Co-deposition in the DIII-D Divertor
Effect of the Surface Temperature on Net Carbon Deposition and Deuterium Co-deposition in the DIII-D Divertor Presented by Dmitry Rudakov (UCSD) for the DiMES Team and Collaborators Presented at the 47th
More informationADVANCES IN PREDICTIVE THERMO-MECHANICAL MODELLING FOR THE JET DIVERTOR EXPERIMENTAL INTERPRETATION, IMPROVED PROTECTION, AND RELIABLE OPERATION
D. IGLESIAS et al. ADVANCES IN PREDICTIVE THERMO-MECHANICAL MODELLING FOR THE JET DIVERTOR EXPERIMENTAL INTERPRETATION, IMPROVED PROTECTION, AND RELIABLE OPERATION D. IGLESIAS CCFE Abingdon, UK Email:
More informationDeuterium Inventory in Tore Supra : reconciling particle balance and post mortem analysis
Deuterium Inventory in Tore Supra : reconciling particle balance and post mortem analysis E. Tsitrone, C. Brosset, B. Pégourié, E. Gauthier, J. Bouvet, J. Bucalossi, S. Carpentier, Y. Corre, E. Delchambre,
More informationPlasma-wall interaction studies in the full-w ASDEX Upgrade during helium plasma discharges
1 P6-349 Plasma-wall interaction studies in the full-w ASDEX Upgrade during helium plasma discharges A. Hakola 1, S. Brezinsek 2, D. Douai 3, M. Balden 4, V. Bobkov 4, D. Carralero 4, H. Greuner 4, A.
More informationTHERMAL OXIDATION EXPERIMENTS TO UNDERSTAND TRITIUM RECOVERY IN DIII-D, JET, C-MOD, AND MAST
GA A25482 13 C-TRACER EXPERIMENTS IN DIII-D PRELIMINARY IN THERMAL OXIDATION EXPERIMENTS TO UNDERSTAND TRITIUM RECOVERY IN DIII-D, JET, C-MOD, AND MAST by P.C. STANGEBY, S.L. ALLEN, N. BEKRIS, N.H. BROOKS,
More informationCritical Gaps between Tokamak Physics and Nuclear Science. Clement P.C. Wong General Atomics
Critical Gaps between Tokamak Physics and Nuclear Science (Step 1: Identifying critical gaps) (Step 2: Options to fill the critical gaps initiated) (Step 3: Success not yet) Clement P.C. Wong General Atomics
More informationTokamak Divertor System Concept and the Design for ITER. Chris Stoafer April 14, 2011
Tokamak Divertor System Concept and the Design for ITER Chris Stoafer April 14, 2011 Presentation Overview Divertor concept and purpose Divertor physics General design considerations Overview of ITER divertor
More informationPISCES W fuzz experiments: A summary of work up to now.
FNST/PFC/MASCO meeting, UCLA Aug. 2-6, 2010 W fuzz experiments: A summary of work up to now. M.J. Baldwin, R.P. Doerner, D. Nishijima University of California, San Diego, USA Why do we care about fuzz?
More informationPlasma-Wall Interaction Studies in the Full-W ASDEX Upgrade during Helium Plasma Discharges
1 EX/P6-21 Plasma-Wall Interaction Studies in the Full-W ASDEX Upgrade during Helium Plasma Discharges A. Hakola 1, S. Brezinsek 2, D. Douai 3, M. Balden 4, V. Bobkov 4, D. Carralero 4, H. Greuner 4, S.
More informationLong Term Reduction of Divertor Carbon Sources in DIII-D
Long Term Reduction of Divertor Carbon Sources in DIII-D D.G Whyte, UCSD R. Doerner, W.P. West, R.L. Lee, N.H. Brooks, R.D. Isler, M.R. Wade, G.D. Porter APS-DPP, Seattle, Nov. 1999 NATIONAL FUSION FACILITY
More informationThermographic measurements of power loads to plasma facing components at Wendelstein 7-X
Thermographic measurements of power loads to plasma facing components at Wendelstein 7-X M.W. Jakubowski 1, A. Ali 1, P. Drewelow 1, H. Niemann 1, F. Pisano 4, A. Puig Sitjes 1, G. Wurden 3, C. Biedermann
More informationList of Papers. P. Petersson, H. Bergsåker, G. Possnert, J.P. Coad, J. Likonen, S. Koivuranta, A. Hakola, and JET-EFDA Contributors
List of Papers This thesis is based on the following papers: I II III IV V VI Measurement of hydrogen isotopes by a nuclear microprobe P. Petersson, J. Jensen, A. Hallén and G. Possnert J. Phys.: Conf.
More informationITER. Power and Particle Exhaust in ITER ITER
Power and Particle Exhaust in ITER ITER G. Janeschitz, C. Ibbott, Y. Igitkhanov, A. Kukushkin, H. Pacher, G. Pacher, R. Tivey, M. Sugihara, JCT and HTs San Diego.5.2 Power and Particle Exhaust in ITER
More informationFusion Plasma Physics Annual Report Division of Fusion Plasma Physics Alfvén Laboratory School of Electrical Engineering KTH
Fusion Plasma Physics Annual Report 2006 Division of Fusion Plasma Physics Alfvén Laboratory School of Electrical Engineering KTH Stockholm, May 2007 Division of Fusion Plasma Physics, Alfvén Laboratory,
More informationDivertor Power Handling Assessment for Baseline Scenario Operation in JET in Preparation for the ILW
EFDA JET CP(9)6/54 I. Nunes, P.J. Lomas, G. Saibene, T. Eich, G. Arnoux, H. Thomsen, E de la Luna and JET EFDA contributors Divertor Power Handling Assessment for Baseline Scenario Operation in JET in
More informationDevelopment of models for plasma interactions with Be on the basis of dedicated experiments
Member of the Helmholtz Association Development of models for plasma interactions with Be on the basis of dedicated experiments D.Borodin 1, A.Kreter 1, A.Huber 1, A.Kirschner 1, S.Brezinsek 1,3, C.Björkas
More informationEffect of ExB Driven Transport on the Deposition of Carbon in the Outer Divertor of. ASDEX Upgrade
Association Euratom-Tekes ASDEX Upgrade Effect of ExB Driven Transport on the Deposition of Carbon in the Outer Divertor of ASDEX Upgrade L. Aho-Mantila 1,2, M. Wischmeier 3, K. Krieger 3, V. Rohde 3,
More informationPlasma Wall Interactions in Tokamak
Plasma Wall Interactions in Tokamak Dr. C Grisolia, Association Euratom/CEA sur la fusion, CEA/Cadarache Outline 1. Conditions for Fusion in Tokamaks 2. Consequences of plasma operation on in vessel materials:
More informationImpurity accumulation in the main plasma and radiation processes in the divetor plasma of JT-60U
1 EX/P4-25 Impurity accumulation in the main plasma and radiation processes in the divetor plasma of JT-6U T. Nakano, H. Kubo, N. Asakura, K. Shimizu and S. Higashijima Japan Atomic Energy Agency, Naka,
More informationOverview of comprehensive characterisation of erosion zones on plasma facing components
Fusion Engineering and Design 81 (2006) 211 219 Overview of comprehensive characterisation of erosion zones on plasma facing components M.J. Rubel a,, E. Fortuna b, A. Kreter c, E. Wessel d, V. Philipps
More informationPlasma-beryllium interactions in ITER: research needs
Plasma-beryllium interactions in ITER: research needs G. De Temmerman a, With contributions from M.J. Baldwin b, D. Anthoine a, K. Heinola c, A. Jan a, I. Jepu d, J. Likonen e, S. Lisgo a C.P. Lungu d,
More informationTungsten: An option for divertor and main chamber PFCs in future fusion devices
ASDEX Upgrade Tungsten: An option for divertor and main chamber PFCs in future fusion devices R. Neu, R. Dux, A. Kallenbach, C.F. Maggi, T. Pütterich, M. Balden, T. Eich, J.C. Fuchs, O. Gruber, A. Herrmann,
More informationComparison of tungsten fuzz growth in Alcator C-Mod and linear plasma devices!
Comparison of tungsten fuzz growth in Alcator C-Mod and linear plasma devices G.M. Wright 1, D. Brunner 1, M.J. Baldwin 2, K. Bystrov 3, R. Doerner 2, B. LaBombard 1, B. Lipschultz 1, G. de Temmerman 3,
More informationDynamic retention and deposition in NSTX measured with quartz microbalances
Supported by Office of Science Dynamic retention and deposition in NSTX measured with quartz microbalances College W&M Colorado Sch Mines Columbia U Comp-X General Atomics INEL Johns Hopkins U LANL LLNL
More informationThe role of PMI in MFE/IFE common research
The role of PMI in MFE/IFE common research Presented by Doerner for the Team and TITAN 1-1 Participants In 2006, Jupiter II recognized that PMI was a bridge issue between MFE and IFE R&D Both MFE and IFE
More informationSTEADY-STATE EXHAUST OF HELIUM ASH IN THE W-SHAPED DIVERTOR OF JT-60U
Abstract STEADY-STATE EXHAUST OF HELIUM ASH IN THE W-SHAPED DIVERTOR OF JT-6U A. SAKASAI, H. TAKENAGA, N. HOSOGANE, H. KUBO, S. SAKURAI, N. AKINO, T. FUJITA, S. HIGASHIJIMA, H. TAMAI, N. ASAKURA, K. ITAMI,
More informationDivertor Requirements and Performance in ITER
Divertor Requirements and Performance in ITER M. Sugihara ITER International Team 1 th International Toki Conference Dec. 11-14, 001 Contents Overview of requirement and prediction for divertor performance
More informationNSTX Plasma-Material Interface (PMI) Probe and supporting experiments
NSTX Plasma-Material Interface (PMI) Probe and supporting experiments J.P. Allain 1,2, C.N. Taylor 1, B. Heim 1,3 PPPL Collaborators: C.H. Skinner, H.W. Kugel, R. Kaita, A.L. Roquemore 1 Purdue University,
More informationEffect ofe B driven transport on the deposition of carbon in the outer divertor of ASDEX Upgrade
Effect ofe B driven transport on the deposition of carbon in the outer divertor of ASDEX Upgrade 0-29 L. Aho-Mantila a,b *, M. Wischmeier c, K. Krieger c, V. Rohde c, H.W. Müller c, D.P. Coster c, M. Groth
More informationPhysics of fusion power. Lecture 14: Anomalous transport / ITER
Physics of fusion power Lecture 14: Anomalous transport / ITER Thursday.. Guest lecturer and international celebrity Dr. D. Gericke will give an overview of inertial confinement fusion.. Instabilities
More informationIsotope Exchange in High Heat-flux Components of the JET Tritium Neutral Beam Injector
JET CP(98)39 Isotope Exchange in High Heat-flux Components of the JET Neutral Beam Injector D Ciric, H P L de Esch, H-D Falter, T T C Jones, L Svensson. JET Joint Undertaking, Abingdon, Oxfordshire, OX14
More informationPower Exhaust on JET: An Overview of Dedicated Experiments
Power Exhaust on JET: An Overview of Dedicated Experiments W.Fundamenski, P.Andrew, T.Eich 1, G.F.Matthews, R.A.Pitts 2, V.Riccardo, W.Sailer 3, S.Sipila 4 and JET EFDA contributors 5 Euratom/UKAEA Fusion
More informationDevelopment of an experimental profile database for the scrape-off layer
Development of an experimental profile database for the scrape-off layer M. Groth, 1 G.D. Porter, 1 W.M. Meyer, 1 A.W. Leonard, 2 T.H. Osborne, 2 D.P. Coster, 3 A. Kallenbach, 3 M. Wischmeier 3 N.H. Brooks,
More informationMaterials for Future Fusion Reactors under Severe Stationary and Transient Thermal Loads
Mitglied der Helmholtz-Gemeinschaft Materials for Future Fusion Reactors under Severe Stationary and Transient Thermal Loads J. Linke, J. Du, N. Lemahieu, Th. Loewenhoff, G. Pintsuk, B. Spilker, T. Weber,
More informationRecent Development of LHD Experiment. O.Motojima for the LHD team National Institute for Fusion Science
Recent Development of LHD Experiment O.Motojima for the LHD team National Institute for Fusion Science 4521 1 Primary goal of LHD project 1. Transport studies in sufficiently high n E T regime relevant
More informationHydrogenic retention of high-z refractory metals exposed to ITER divertor relevant plasma conditions
1 Hydrogenic retention of high-z refractory metals exposed to ITER divertor relevant plasma conditions G.M. Wright 1), E. Alves 2), L.C. Alves 2), N.P. Barradas 2), M. Mayer 3), G.J. van Rooij 1), R.S.
More informationFusion Plasma Physics Annual Report Fusion Plasma Physics School of Electrical Engineering KTH Royal Institute of Technology
Fusion Plasma Physics Annual Report 2013 Fusion Plasma Physics School of Electrical Engineering KTH Royal Institute of Technology Stockholm, December 2014 Fusion Plasma Physics School of Electrical Engineering
More informationExperimental results and modelling of ASDEX Upgrade partial detachment
Experimental results and modelling of ASDEX Upgrade partial detachment M. Wischmeier 1 With thanks to X. Bonnin 2, P. Börner 3, A. Chankin 1, D. P. Coster 1, M. Groth 4, A. Kallenbach 1, V. Kotov 3, H.
More informationTemporal Evolution and Spatial Distribution of Dust Creation Events in Tore Supra and in ASDEX Upgrade Studied by CCD Image Analysis
Temporal Evolution and Spatial Distribution of Dust Creation Events in Tore Supra and in ASDEX Upgrade Studied by CCD Image Analysis Suk-Ho Hong 1,, Christian Grisolia 2, Volker Rohde 3, Pascale Monier-Garbet
More informationMission Elements of the FNSP and FNSF
Mission Elements of the FNSP and FNSF by R.D. Stambaugh PERSISTENT SURVEILLANCE FOR PIPELINE PROTECTION AND THREAT INTERDICTION Presented at FNST Workshop August 3, 2010 In Addition to What Will Be Learned
More informationInfluence of gas impuritites on plasma performance on JET tokamak
19 Influence of gas impuritites on plasma performance on JET tokamak Martin Kubič České vysoké učení technické v Praze Fakulta jaderná a fyzikálně inženýrská Katedra fyziky THERMONUCLEAR FUSION 1.1 Introduction
More informationMax-Planck-Institut für Plasmaphysik, EURATOM Association POB 1533, D Garching, Germany
DEPTH PROFILE REONSTRUTION FROM RUTHERFORD BAKSATTERING DATA U. V. TOUSSAINT, K. KRIEGER, R. FISHER, V. DOSE Max-Planck-Institut für Plasmaphysik, EURATOM Association POB 1533, D-8574 Garching, Germany
More informationAnalyses of Visible Images of the Plasma Periphery Observed with Tangentially Viewing CCD Cameras in the Large Helical Device
Analyses of Visible Images of the Plasma Periphery Observed with Tangentially Viewing CCD Cameras in the Large Helical Device M. SHOJI, T. WATANABE, S. MASUZAKI, H. YAMADA, A. KOMORI and LHD Experimental
More informationand expectations for the future
39 th Annual Meeting of the FPA 2018 First operation of the Wendelstein 7-X stellarator and expectations for the future Hans-Stephan Bosch Max-Planck-Institut für Plasmaphysik Greifswald, Germany on behalf
More informationThe emissivity of W coatings deposited on carbon materials for fusion applications
EUROFUSION WPJET2-CP(16) 15583 C Ruset et al. The emissivity of W coatings deposited on carbon materials for fusion applications Preprint of Paper to be submitted for publication in Proceedings of 29th
More informationCan we tend the fire?
Can we tend the fire? Three lectures course on plasma surface interaction and edge physics II.) HOW can we make the application work (build ITER)? Detlev Reiter Forschungszentrum Jülich GmbH, Institut
More informationModeling Plasma Interactions with ITER Wall Materials: Erosion, Transport, Redeposition, Reerosion and Material Mixing, and Tritium Retention
Modeling Plasma Interactions with ITER Wall Materials: Erosion, Transport, Redeposition, Reerosion and Material Mixing, and Tritium Retention Kaoru Ohya Institute of Technology and Science, The University
More informationARTICLES PLASMA DETACHMENT IN JET MARK I DIVERTOR EXPERIMENTS
ARTICLES PLASMA DETACHMENT IN JET MARK I DIVERTOR EXPERIMENTS A. LOARTE, R.D. MONK, J.R. MARTÍN-SOLÍSa,D.J.CAMPBELL, A.V. CHANKIN b, S. CLEMENT, S.J. DAVIES, J. EHRENBERG, S.K. ERENTS c,h.y.guo, P.J. HARBOUR,
More informationChemical Sputtering of Carbon Materials due to Combined Bombardment by Ions and Atomic Hydrogen
Chemical Sputtering of Carbon Materials due to Combined Bombardment by Ions and Atomic Hydrogen W. Jacob, C. Hopf, and M. Schlüter Max-Planck-Institut für Plasmaphysik, EURATOM Association, Boltzmannstr.
More informationDIVIMP simulation of W transport in the SOL of JET H-mode plasmas
DIVIMP simulation of W transport in the SOL of JET H-mode plasmas A. Järvinen a, C. Giroud b, M. Groth a, K. Krieger c, D. Moulton d, S. Wiesen e, S. Brezinsek e and JET- EFDA contributors¹ JET-EFDA, Culham
More informationDriving Mechanism of SOL Plasma Flow and Effects on the Divertor Performance in JT-60U
EX/D-3 Driving Mechanism of SOL Plasma Flow and Effects on the Divertor Performance in JT-6U N. Asakura ), H. Takenaga ), S. Sakurai ), G.D. Porter ), T.D. Rognlien ), M.E. Rensink ), O. Naito ), K. Shimizu
More informationElastic Recoil Detection Method using DT Neutrons for Hydrogen Isotope Analysis in Fusion Materials. Abstract
Elastic Recoil Detection Method using DT Neutrons for Hydrogen Isotope Analysis in Fusion Materials Naoyoshi Kubota, Kentaro Ochiai, Keitaro Kondo 2 and Takeo Nishitani. :Japan Atomic Energy Research Institute,
More informationEFDA European Fusion Development Agreement - Close Support Unit - Garching
Multi-machine Modelling of Divertor Geometry Effects Alberto Loarte EFDA CSU -Garching Acknowledgements: K. Borrass, D. Coster, J. Gafert, C. Maggi, R. Monk, L. Horton, R.Schneider (IPP), A.Kukushkin (ITER),
More informationEROSION AND DEPOSITION MECHANISMS IN FUSION PLASMAS. A. Kirschner
EROSION AND DEPOSITION MECHANISMS IN FUSION PLASMAS A. Kirschner Institut für Energieforschung (Plasmaphysik), Forschungszentrum Jülich GmbH, Association EURATOM-FZJ, Trilateral Euregio Cluster, 52425
More informationCross-Field Transport in the SOL: Its Relationship to Main Chamber and Divertor Neutral Control in Alcator C-Mod
Cross-Field Transport in the SOL: Its Relationship to Main Chamber and Divertor Neutral Control in Alcator C-Mod B. LaBombard, B. Lipschultz, J.A. Goetz, C.S. Pitcher, N. Asakura 1), R.L. Boivin, J.W.
More informationEstimating the plasma flow in a recombining plasma from
Paper P3-38 Estimating the plasma flow in a recombining plasma from the H α emission U. Wenzel a, M. Goto b a Max-Planck-Institut für Plasmaphysik (IPP) b National Institute for Fusion Science, Toki 509-5292,
More informationAir exposure and sample storage time influence on hydrogen release from tungsten
Air exposure and sample storage time influence on hydrogen release from tungsten K.A. Moshkunov a, K. Schmid b, M. Mayer b, V.A. Kurnaev a, Yu.M. Gasparyan a a National research nuclear university MEPhI,
More informationScaling of divertor heat flux profile widths in DIII-D
1 Scaling of divertor heat flux profile widths in DIII-D C.J. Lasnier 1, M.A. Makowski 1, J.A. Boedo 2, N.H. Brooks 3, D.N. Hill 1, A.W. Leonard 3, and J.G. Watkins 4 e-mail:lasnier@llnl.gov 1 Lawrence
More informationHighlights from (3D) Modeling of Tokamak Disruptions
Highlights from (3D) Modeling of Tokamak Disruptions Presented by V.A. Izzo With major contributions from S.E. Kruger, H.R. Strauss, R. Paccagnella, MHD Control Workshop 2010 Madison, WI ..onset of rapidly
More informationDiagnostics for Burning Plasma Physics Studies: A Status Report.
Diagnostics for Burning Plasma Physics Studies: A Status Report. Kenneth M. Young Princeton Plasma Physics Laboratory UFA Workshop on Burning Plasma Science December 11-13 Austin, TX Aspects of Plasma
More informationBe tile power handling and main wall protection
Be tile power handling and main wall protection I Nunes 1, V Riccardo 2, P J Lomas 2, P de Vries 3, D Alves 1, G Arnoux 4, S Devaux 2, T Farley 5, M Firdaouss 6, S Jachmich 7, G Matthews 2, C Reux 8, K-D
More informationDevelopment of Langmuir Probes on Divertor Cassettes in JT-60SA
Development of Langmuir Probes on Divertor Cassettes in JT-60SA Masakatsu FUKUMOTO, Shinji SAKURAI, Nobuyuki ASAKURA 1) and Kiyoshi ITAMI Japan Atomic Energy Agency, Naka, Ibaraki 311-0193, Japan 1) Japan
More informationABSTRACT, POSTER LP1 12 THURSDAY 11/7/2001, APS DPP CONFERENCE, LONG BEACH. Recent Results from the Quiescent Double Barrier Regime on DIII-D
ABSTRACT, POSTER LP1 1 THURSDAY 11/7/1, APS DPP CONFERENCE, LONG BEACH Recent Results from the Quiescent Double Barrier Regime on DIII-D E.J. Doyle, K.H. Burrell, T. Casper, J.C. DeBoo, A. Garofalo, P.
More informationModelling Erosion and Redeposition on Plasma Facing Walls: Basics and Recent progress
Joint ICTP-IAEA Workshop on Fusion Plasma Modelling Using Atomic and Molecular Data, Trieste, Italy, 23-27 January 22 Modelling Erosion and Redeposition on Plasma Facing Walls: Basics and Recent progress
More informationHydrogen and Helium Edge-Plasmas
Hydrogen and Helium Edge-Plasmas Comparison of high and low recycling T.D. Rognlien and M.E. Rensink Lawrence Livermore National Lab Presented at the ALPS/APEX Meeting Argonne National Lab May 8-12, 2
More informationFAR SCRAPE-OFF LAYER AND NEAR WALL PLASMA STUDIES IN DIII D
GA A24724 FAR SCRAPE-OFF LAYER AND NEAR WALL PLASMA STUDIES IN DIII D by D.L. RUDAKOV, J.A. BOEDO, R.A. MOYER, N.H. BROOKS, R.P. DOERNER, T.E. EVANS, M.E. FENSTERMACHER, M. GROTH, E.M. HOLLMANN, S. KRASHENINNIKOV,
More informationFusion Plasma Physics Annual Report Division of Fusion Plasma Physics School of Electrical Engineering KTH
Fusion Plasma Physics Annual Report 2007 Division of Fusion Plasma Physics School of Electrical Engineering KTH Stockholm, May 2008 Division of Fusion Plasma Physics School of Electrical Engineering KTH
More informationSome Notes on the Window Frame Method for Assessing the Magnitude and Nature of Plasma-Wall Contact
Some Notes on the Window Frame Method for Assessing the Magnitude and Nature of Plasma-Wall Contact Peter Stangeby 4 September 2003 1. Fig. 1 shows an example of a suitable magnetic configuration for application
More informationRecent results in dynamic retention and dust
Recent results in dynamic retention and dust Charles Skinner, Lane Roquemore, Henry Kugel, PPPL Rajesh Maingi, ORNL, William Wampler, SNL, with National Undergraduate Fellows: Aaron Bader, Cooper Union,
More informationElectrical Characterization with SPM Application Modules
Electrical Characterization with SPM Application Modules Metrology, Characterization, Failure Analysis: Data Storage Magnetoresistive (MR) read-write heads Semiconductor Transistors Interconnect Ferroelectric
More informationDivertor Heat Flux Reduction and Detachment in NSTX
1 EX/P4-28 Divertor Heat Flux Reduction and Detachment in NSTX V. A. Soukhanovskii 1), R. Maingi 2), R. Raman 3), R. E. Bell 4), C. Bush 2), R. Kaita 4), H. W. Kugel 4), C. J. Lasnier 1), B. P. LeBlanc
More informationImplantation Energy Dependence on Deuterium Retention Behaviors for the Carbon Implanted Tungsten
J. Plasma Fusion Res. SERIES, Vol. 10 (2013) Implantation Energy Dependence on Deuterium Retention Behaviors for the Carbon Implanted Tungsten Yasuhisa Oya 1) *, Makoto Kobayashi 1), Naoaki Yoshida 2),
More information