1. Comparison of ITER performance predicted by semi-empirical and theory-based transport models
- Author
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A. Polevoi, M. Sugihara, J. G. Cordey, A. Kukushkin, O. Zolotukhin, G. V. Pereverzev, Arnold H. Kritz, G. Bateman, Alexei Pankin, I. Voitsekhovich, Jan Weiland, F. W. Perkins, Y. Shimomura, A. Chudnovskiy, V. Mukhovatov, Thawatchai Onjun, M. Shimada, and O. Kardaun
- Subjects
Physics ,Nuclear and High Energy Physics ,Jet (fluid) ,Magnetic confinement fusion ,chemistry.chemical_element ,Plasma ,Mechanics ,Fusion power ,Condensed Matter Physics ,Power (physics) ,Nuclear physics ,Pedestal ,chemistry ,Scaling ,Helium - Abstract
The values of Q = (fusion power)/(auxiliary heating power) predicted for ITER by three different methods are compared. The first method utilizes an empirical confinement-time scaling and prescribed radial profiles of transport coefficients; the second approach extrapolates from specially designed ITER similarity experiments, and the third approach is based on partly theory-based transport models. The energy confinement time given by the ITERH-98(y, 2) scaling for an inductive scenario with a plasma current of 15 MA and a plasma density 15% below the Greenwald density is 3.7 s with one estimated technical standard deviation of ±14%. This translates, in the first approach, for levels of helium removal, and impurity concentration, that, albeit rather stringent, are expected to be attainable, into an interval for Q of [6–15] at the auxiliary heating power, Paux = 40 MW, and [6–30] at the minimum heating power satisfying a good confinement ELMy H-mode. All theoretical transport-model calculations have been performed for the plasma core only, whereas the pedestal temperatures were taken as estimated from empirical scalings. Predictions of similarity experiments from JET and of theory-based transport models that we have considered—Weiland, MMM, and IFS/PPPL—overlap with the prediction using the empirical confinement-time scaling within its estimated margin of uncertainty.
- Published
- 2003
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