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  Characteristics of the H-mode pedestal and extrapolation to ITER

Osborne, T. H., Cordey, J. G., Groebner, R. J., Hatae, T., Hubbard, A., Horton, L. D., et al. (2003). Characteristics of the H-mode pedestal and extrapolation to ITER. In Fusion Energy 2002. Vienna: International Atomic Energy Agency.

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 Creators:
Osborne, T. H.1, Author
Cordey, J. G.1, Author
Groebner, R. J.1, Author
Hatae, T.1, Author
Hubbard, A.1, Author
Horton, L. D.2, Author           
Kamada, Y.1, Author
Kritz, A.1, Author
Lao, L. L.1, Author
Leonard, A. W.1, Author
Loarte, A.1, Author
Mahdavi, M. A.1, Author
Mossessian, D.1, Author
Onjun, T.1, Author
Ossenpenko, M.1, Author
Rognlien, T. D.1, Author
Saibene, G.1, Author
Snyder, P. B.1, Author
Sugihara, M.3, Author           
Shurygin, R.1, Author
Thomsen, K.1, AuthorWade, M. R.1, AuthorWilson, H. R.1, AuthorXu, X. Q.1, AuthorYatsu, K.1, AuthorInternational Tokamak Physics Activity H Mode Pedestal Working Group1, Author more..
Affiliations:
1General Atomics, San Diego, CA, USA; EURATOM/UKAEA Fusion Association, Culham Science Center, Abingdon, United Kingdom ; Japan Atomic Energy Research Institute, Naka-machi, Ibaraki-ken, Japan ; Massachusetts Institute of Technology, Cambridge, Massachusetts USA; Lehigh University, Bethlehem, Pennsylvania USA; EFDA-JET, Culham, United Kingdom; Institute of Nuclear Fusion, Kurchatov Institute, Russia; Lawrence Livermore National Laboratory, Livermore, California, USA; ITER Joint Work Site, Naka, Japan; Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA; Plasma Research Center, University of Tsukuba, Tsukuba, Ibaraki, Japan, ou_persistent22              
2Experimental Plasma Physics 1 (E1), Max Planck Institute for Plasma Physics, Max Planck Society, ou_1856295              
3Experimental Plasma Physics 2 (E2), Max Planck Institute for Plasma Physics, Max Planck Society, ou_1856292              

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 Abstract: The development of a predictive capability for the characteristics of the H-mode pedestal and ELMs is important in predicting tokamak reactor performance. The H-mode pedestal effects core confinement through temperature profile stiffness. The ELM power flux can significantly impact divertor design. We discuss progress in these areas through inter-machine comparison under the venue of the International Tokamak Physics Activity, ITPA. The pressure in the H-mode transport barrier region is typically set by the ELM cycle rather than transport. Several features of the ELM onset conditions are consistent with an ideal peeling-ballooning mode instability: 1) strong shape dependence, 2) mode structure, 3) reduced p' at high collisionality, 4) p' dependence on transport barrier width. Type I ELM energy loss is found to be proportional to the energy in the H-mode pedestal. There is some consistency between the peeling-ballooning mode radial width and the ELM size. Type I ELM energy loss is reduced at high density to levels that would be tolerable in a reactor scale device through reduced conductive loss and possibly shift to a more radially localized instability.

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Language(s): eng - English
 Dates: 2003
 Publication Status: Issued
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 Rev. Type: Internal
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Title: 19th Fusion Energy Conference
Place of Event: Lyon (FR)
Start-/End Date: 2002-10-14 - 2002-10-19

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Title: Fusion Energy 2002
Source Genre: Proceedings
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Publ. Info: Vienna : International Atomic Energy Agency
Pages: CD-ROM Volume / Issue: - Sequence Number: CT-3 Start / End Page: - Identifier: -