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Dive into the research topics where C.H. Skinner is active.

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Featured researches published by C.H. Skinner.


Nuclear Fusion | 2001

Plasma{material interactions in current tokamaks and their implications for next step fusion reactors

G. Federici; C.H. Skinner; J.N. Brooks; J. P. Coad; C. Grisolia; A.A. Haasz; A. Hassanein; V. Philipps; C. S. Pitcher; J. Roth; W.R. Wampler; D.G. Whyte

The major increase in discharge duration and plasma energy in a next step DT fusion reactor will give rise to important plasma-material effects that will critically influence its operation, safety and performance. Erosion will increase to a scale of several centimetres from being barely measurable at a micron scale in todays tokamaks. Tritium co-deposited with carbon will strongly affect the operation of machines with carbon plasma facing components. Controlling plasma-wall interactions is critical to achieving high performance in present day tokamaks, and this is likely to continue to be the case in the approach to practical fusion reactors. Recognition of the important consequences of these phenomena stimulated an internationally co-ordinated effort in the field of plasma-surface interactions supporting the Engineering Design Activities of the International Thermonuclear Experimental Reactor project (ITER), and significant progress has been made in better understanding these issues. The paper reviews the underlying physical processes and the existing experimental database of plasma-material interactions both in tokamaks and laboratory simulation facilities for conditions of direct relevance to next step fusion reactors. Two main topical groups of interaction are considered: (i) erosion/redeposition from plasma sputtering and disruptions, including dust and flake generation and (ii) tritium retention and removal. The use of modelling tools to interpret the experimental results and make projections for conditions expected in future devices is explained. Outstanding technical issues and specific recommendations on potential R&D avenues for their resolution are presented.


Journal of Nuclear Materials | 1999

In-vessel tritium retention and removal in ITER

G. Federici; R.A. Anderl; P.L. Andrew; J.N. Brooks; R.A. Causey; J. P. Coad; D. Cowgill; R.P. Doerner; A.A. Haasz; G. Janeschitz; W. Jacob; G.R. Longhurst; R. Nygren; A.T. Peacock; M.A. Pick; V. Philipps; J. Roth; C.H. Skinner; W.R. Wampler

Abstract Tritium retention inside the vacuum vessel has emerged as a potentially serious constraint in the operation of the International Thermonuclear Experimental Reactor (ITER). In this paper we review recent tokamak and laboratory data on hydrogen, deuterium and tritium retention for materials and conditions which are of direct relevance to the design of ITER. These data, together with significant advances in understanding the underlying physics, provide the basis for modelling predictions of the tritium inventory in ITER. We present the derivation, and discuss the results, of current predictions both in terms of implantation and codeposition rates, and critically discuss their uncertainties and sensitivity to important design and operation parameters such as the plasma edge conditions, the surface temperature, the presence of mixed-materials, etc. These analyses are consistent with recent tokamak findings and show that codeposition of tritium occurs on the divertor surfaces primarily with carbon eroded from a limited area of the divertor near the strike zones. This issue remains an area of serious concern for ITER. The calculated codeposition rates for ITER are relatively high and the in-vessel tritium inventory limit could be reached, under worst assumptions, in approximately a week of continuous operation. We discuss the implications of these estimates on the design, operation and safety of ITER and present a strategy for resolving the issues. We conclude that as long as carbon is used in ITER – and more generically in any other next-step experimental fusion facility fuelled with tritium – the efficient control and removal of the codeposited tritium is essential. There is a critical need to develop and test in situ cleaning techniques and procedures that are beyond the current experience of present-day tokamaks. We review some of the principal methods that are being investigated and tested, in conjunction with the R&D work still required to extrapolate their applicability to ITER. Finally, unresolved issues are identified and recommendations are made on potential R&D avenues for their resolution.


Review of Scientific Instruments | 2008

Dust measurements in tokamaks (invited)

D.L. Rudakov; J.H. Yu; J.A. Boedo; E.M. Hollmann; S. I. Krasheninnikov; R.A. Moyer; S.H. Muller; A. Yu. Pigarov; M. Rosenberg; R.D. Smirnov; W.P. West; R. L. Boivin; B.D. Bray; N.H. Brooks; A.W. Hyatt; C.P.C. Wong; A.L. Roquemore; C.H. Skinner; W.M. Solomon; Svetlana V. Ratynskaia; M.E. Fenstermacher; M. Groth; C.J. Lasnier; A.G. McLean; P.C. Stangeby

Dust production and accumulation present potential safety and operational issues for the ITER. Dust diagnostics can be divided into two groups: diagnostics of dust on surfaces and diagnostics of dust in plasma. Diagnostics from both groups are employed in contemporary tokamaks; new diagnostics suitable for ITER are also being developed and tested. Dust accumulation in ITER is likely to occur in hidden areas, e.g., between tiles and under divertor baffles. A novel electrostatic dust detector for monitoring dust in these regions has been developed and tested at PPPL. In the DIII-D tokamak dust diagnostics include Mie scattering from Nd:YAG lasers, visible imaging, and spectroscopy. Laser scattering is able to resolve particles between 0.16 and 1.6 microm in diameter; using these data the total dust content in the edge plasmas and trends in the dust production rates within this size range have been established. Individual dust particles are observed by visible imaging using fast framing cameras, detecting dust particles of a few microns in diameter and larger. Dust velocities and trajectories can be determined in two-dimension with a single camera or three-dimension using multiple cameras, but determination of particle size is challenging. In order to calibrate diagnostics and benchmark dust dynamics modeling, precharacterized carbon dust has been injected into the lower divertor of DIII-D. Injected dust is seen by cameras, and spectroscopic diagnostics observe an increase in carbon line (CI, CII, C(2) dimer) and thermal continuum emissions from the injected dust. The latter observation can be used in the design of novel dust survey diagnostics.


Nuclear Fusion | 2009

Principal physics developments evaluated in the ITER design review

R.J. Hawryluk; D.J. Campbell; G. Janeschitz; P.R. Thomas; R. Albanese; R. Ambrosino; C. Bachmann; L. R. Baylor; M. Becoulet; I. Benfatto; J. Bialek; Allen H. Boozer; A. Brooks; R.V. Budny; T.A. Casper; M. Cavinato; J.-J. Cordier; V. Chuyanov; E. J. Doyle; T.E. Evans; G. Federici; M.E. Fenstermacher; H. Fujieda; K. Gál; A. M. Garofalo; L. Garzotti; D.A. Gates; Y. Gribov; P. Heitzenroeder; T. C. Hender

As part of the ITER Design Review and in response to the issues identified by the Science and Technology Advisory Committee, the ITER physics requirements were reviewed and as appropriate updated. The focus of this paper will be on recent work affecting the ITER design with special emphasis on topics affecting near-term procurement arrangements. This paper will describe results on: design sensitivity studies, poloidal field coil requirements, vertical stability, effect of toroidal field ripple on thermal confinement, material choice and heat load requirements for plasma-facing components, edge localized modes control, resistive wall mode control, disruptions and disruption mitigation.


Nuclear Fusion | 2001

Equilibrium properties of spherical torus plasmas in NSTX

Steven Anthony Sabbagh; S.M. Kaye; J. Menard; F. Paoletti; M.G. Bell; R.E. Bell; J. Bialek; M. Bitter; E.D. Fredrickson; D.A. Gates; A.H. Glasser; H.W. Kugel; L. L. Lao; Benoit P. Leblanc; R. Maingi; Ricardo Jose Maqueda; E. Mazzucato; D. Mueller; M. Ono; S.F. Paul; M. J. Peng; C.H. Skinner; D. Stutman; G. A. Wurden; W. Zhu

Research in NSTX has been conducted to establish spherical torus plasmas to be used for high ?, auxiliary heated experiments. This device has a major radius R0 = 0.86?m and a midplane halfwidth of 0.7?m. It has been operated with toroidal magnetic field B0 ? 0.3?T and Ip ? 1.0?MA. The evolution of the plasma equilibrium is analysed between discharges with an automated version of the EFIT code. Limiter, double null and lower single null diverted configurations have been sustained for several energy confinement times. The plasma stored energy reached 92?kJ (?t = 17.8%) with neutral beam heating. A plasma elongation in the range 1.6 ? ? ? 2.0 and a triangularity in the range 0.25 ? ? ? 0.45 have been sustained, with values of ? = 2.6 and ? = 0.6 being reached transiently. The reconstructed magnetic signals are fitted to the corresponding measured values with low errors. Aspects of the plasma boundary, pressure and safety factor profiles are supported by measurements from non-magnetic diagnostics. Plasma densities have reached 0.8 and 1.2 times the Greenwald limit in deuterium and helium plasmas, respectively, with no clear limit encountered. Instabilities including sawteeth and reconnection events, characterized by Mirnov oscillations, and a perturbation of the Ip, ? and li evolutions, have been observed. A low q limit was observed and is imposed by a low toroidal mode number kink instability.


Nuclear Fusion | 2007

Plasma?surface interaction, scrape-off layer and divertor physics: implications for ITER

B. Lipschultz; X. Bonnin; G. Counsell; A. Kallenbach; A. Kukushkin; K. Krieger; A.W. Leonard; A. Loarte; R. Neu; R. Pitts; T.D. Rognlien; J. Roth; C.H. Skinner; J. L. Terry; E. Tsitrone; D.G. Whyte; Stewart J. Zweben; N. Asakura; D. Coster; R.P. Doerner; R. Dux; G. Federici; M.E. Fenstermacher; W. Fundamenski; Ph. Ghendrih; A. Herrmann; J. Hu; S. I. Krasheninnikov; G. Kirnev; A. Kreter

Recent research in scrape-off layer (SOL) and divertor physics is reviewed; new and existing data from a variety of experiments have been used to make cross-experiment comparisons with implications for further research and ITER. Studies of the region near the separatrix have addressed the relationship of profiles to turbulence as well as the scaling of the parallel power flow. Enhanced low-field side radial transport is implicated as driving parallel flows to the inboard side. The medium-n nature of edge localized modes (ELMs) has been elucidated and new measurements have determined that they carry ~10?20% of the ELM energy to the far SOL with implications for ITER limiters and the upper divertor. The predicted divertor power loads for ITER disruptions are reduced while those to main chamber plasma facing components (PFCs) increase. Disruption mitigation through massive gas puffing is successful at reducing PFC heat loads. New estimates of ITER tritium retention have shown tile sides to play a significant role; tritium cleanup may be necessary every few days to weeks. ITERs use of mixed materials gives rise to a reduction of surface melting temperatures and chemical sputtering. Advances in modelling of the ITER divertor and flows have enhanced the capability to match experimental data and predict ITER performance.


Fusion Science and Technology | 2008

Recent advances on hydrogen retention in ITER's plasma-facing materials: Beryllium, carbon and tungsten

C.H. Skinner; A.A. Haasz; V.Kh. Alimov; N. Bekris; R.A. Causey; R. E. H. Clark; J. P. Coad; J. W. Davis; R.P. Doerner; M. Mayer; A. Pisarev; J. Roth; T. Tanabe

Abstract Management of tritium inventory remains one of the grand challenges in the development of fusion energy, and the choice of plasma-facing materials is a key factor for in-vessel tritium retention. The Atomic and Molecular Data Unit of the International Atomic Energy Agency organized a Coordinated Research Project (CRP) on the overall topic of tritium inventory in fusion reactors during the period 2001-2006. This dealt with hydrogenic retention in ITER’s plasma-facing materials – Be, C, and W – and in compounds (mixed materials) of these elements as well as tritium removal techniques. The results of the CRP are summarized in this paper together with recommendations for ITER. Basic parameters of diffusivity, solubility, and trapping in Be, C, and W are reviewed. For Be, the development of open porosity can account for transient hydrogenic pumping, but long-term retention will be dominated by codeposition. Codeposition is also the dominant retention mechanism for carbon and remains a serious concern for both Be- and C-containing layers. Hydrogenic trapping in unirradiated tungsten is low but will increase with ion and neutron damage. Mixed materials will be formed in a tokamak, and these can also retain significant amounts of hydrogen isotopes. Oxidative and photon-based techniques for detritiation of plasma-facing components are described.


Journal of Nuclear Materials | 2003

Tritium retention of plasma facing components in tokamaks

T. Tanabe; N. Bekris; P. Coad; C.H. Skinner; M. Glugla; N. Miya

Abstract The areal distribution of tritium retention in tiles from TEXTOR, TFTR, JT-60U and JET has been measured via the imaging plate technique and the results are discussed from the perspective of carbon–hydrogen chemistry. It is found that the observed tritium distribution clearly shows asymmetries in poloidal and toroidal directions and also reflects the local temperature history of the analyzed tiles. We show the first clear evidence of the loss of high energy tritons by toroidal magnetic field ripple. We distinguish three different contributions to tritium retention in tokamaks with carbon plasma facing components: high energy tritons escaping from the core plasma, low energy ions and neutrals from the edge plasma, and molecular tritium from gas fueling. These components are retained at different depths and with different concentrations. Tritium from the edge plasma dominates the retained inventory but could be reduced if the surface temperature was higher. We propose tokamak operation with plasma facing components above 1000 K as a possible way to reduce the tritium inventory.


Plasma Physics and Controlled Fusion | 2001

Initial results from coaxial helicity injection experiments in NSTX

R. Raman; Thomas R. Jarboe; D. Mueller; M.J. Schaffer; Ricardo Jose Maqueda; B.A. Nelson; S.A. Sabbagh; M.G. Bell; R. Ewig; E.D. Fredrickson; D.A. Gates; J. Hosea; Hantao Ji; R. Kaita; S.M. Kaye; H.W. Kugel; R. Maingi; J. Menard; M. Ono; D. Orvis; F. Paoletti; S. Paul; M. J. Peng; C.H. Skinner; J. B. Wilgen; S. J. Zweben

Coaxial helicity injection has been investigated on the National Spherical Torus Experiment (NSTX). Initial experiments produced 130 kA of toroidal current without the use of the central solenoid. The corresponding injector current was 20 kA. Discharges with pulse lengths up to 130 ms have been produced.


Nuclear Fusion | 2001

Non-inductive current generation in NSTX using coaxial helicity injection

R. Raman; Thomas R. Jarboe; D. Mueller; M.J. Schaffer; Ricardo Jose Maqueda; B.A. Nelson; S.A. Sabbagh; M.G. Bell; R. Ewig; E.D. Fredrickson; D.A. Gates; J. C. Hosea; Stephen C. Jardin; Hantao Ji; R. Kaita; S.M. Kaye; H.W. Kugel; L. L. Lao; R. Maingi; J. Menard; M. Ono; D. Orvis; F. Paoletti; S. Paul; Yueng Kay Martin Peng; C.H. Skinner; J. B. Wilgen; S. J. Zweben

Coaxial helicity injection (CHI) on the National Spherical Torus Experiment (NSTX) has produced 240 kA of toroidal current without the use of the central solenoid. Values of the current multiplication ratio (CHI produced toroidal current/injector current) up to 10 were obtained, in agreement with predictions. The discharges, which lasted for up to 200 ms, limited only by the programmed waveform, are more than an order of magnitude longer in duration than any CHI discharges previously produced in a spheromak or a spherical torus.

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H.W. Kugel

Princeton Plasma Physics Laboratory

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R. Kaita

Princeton Plasma Physics Laboratory

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A.L. Roquemore

Princeton Plasma Physics Laboratory

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R. Maingi

Oak Ridge National Laboratory

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M.G. Bell

Princeton Plasma Physics Laboratory

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D. Mueller

Princeton Plasma Physics Laboratory

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Benoit P. Leblanc

Princeton Plasma Physics Laboratory

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J. Menard

Princeton Plasma Physics Laboratory

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R.E. Bell

Princeton Plasma Physics Laboratory

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