Jul 2 – 6, 2018
Žofín Palace
Europe/Prague timezone

P1.1084 Characterization of isotope effect on confinement of NBI-heated plasmas on LHD

Jul 2, 2018, 2:00 PM
2h
Mánes

Mánes

Masarykovo nábřeží 1, 110 00 Praha 1

Speaker

Hiroshi Yamada

Description

See the full Abstract at http://ocs.ciemat.es/EPS2018ABS/pdf/P1.1084.pdf Characterization of Isotope Effect on Confinement of NBI-Heated Plasmas on LHD H. Yamada1,2, K.Tanaka1,3, T.Tokuzawa1, R.Seki1,4, C.Suzuki1, M.Yokoyama1,4, K.Ida1,4, M.Yoshinuma1, K.Fujii5, S.Murakami5 and LHD Experiment Group 1 National Institute for Fusion Science/NINS, Toki, Japan 2 The Univ. Tokyo, Kashiwa, Japan, 3 Kyushu Univ., Kasuga, Japan, 4 SOKENDAI, Toki, Japan, 5Kyoto Univ., Kyoto, Japan Energy confinement and thermal transport has been widely regarded as gyro-Bohm in tokamak as well as stellarator-heliotron for a single kind of ion. However, this gyro-Bohm model predicts confinement degradation in deuterium (D) plasmas because of larger normalized gyro radius * than in hydrogen (H) plasmas, which conflicts with major experimental observations. This study aims to quantify a peculiarity in dependence on * in H and D plasmas in order to address this unresolved issue. The first deuterium plasma campaign in LHD reveals characteristics of isotope effect from elaborated experiments on NBI-heated plasmas. Thermal energy confinement time gives the regression expression scaling with the isotope mass (A) as A0.15, which shows moderate improvement in D plasmas. This positive isotope dependence contradicts with gyro-Bohm and is similar to the recent result from L-mode plasmas in JET-ILW. Operational flexibility of magnetic field, density, and heating power enables adjustment of three major non-dimensional parameters, those being *, collisionality * and  , and dimensionally similar plasmas of H and D in all these three parameters can be obtained. Then TASK3D-a / FIT3D is used for analysis of heating power deposition, power balance and local thermal transport. If gyro-Bohm nature predominates in these plasmas, thermal diffusivity normalized by Bohm diffusion should be the same in a pair of dimensionally similar plasmas of H and D. Different characteristics from this conjecture have been found in electron and ion loss channels. Electron heat diffusivity normalized by Bohm diffusion in H is lower than that in D and even lower by more than a factor of 1/2 which means net improvement. This trend is robust and insensitive to parameters such as *, *,  and Ln. In contrast, ion thermal diffusivity shows same characteristics in low collsionality regime while that in D compared with the case with H degrades with the increase of collsionality. These results have shown definitively that the gyro-Bohm nature is violated in the comparison of H and D plasmas in LHD.

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