1993
DOI: 10.1088/0741-3335/35/sb/026
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Transport in stellarators

Abstract: The local electron and ion heat transport as well as the particle and impurity transport properties in stellaratoa are reviewed. In this context, neoclassical theory is used as a guideline for the comparison of the experimentd results of the quite different confinement concepts. At sufficiently high temperatures depending on the speci6c magnetic configuration, neoelsssical predictions are mfimed by experimental findings. The confinement properties in the LMFP collisionality regime are discussed with respect to… Show more

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Cited by 61 publications
(50 citation statements)
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“…The neoclassically predicted ambipolar radial electric field is generally in agreement with observations in the core of CHS [26] and W7-AS [27,28,29,30] in the 'ion root' regime. Agreement has also been obtained in plasmas with net toroidal current and significant magnetic shear in W7-AS [31], and qualitative agreement has been reported in TJ-II [32].…”
Section: Neoclassical Transport In Stellarators: Theory and Experimentssupporting
confidence: 82%
“…The neoclassically predicted ambipolar radial electric field is generally in agreement with observations in the core of CHS [26] and W7-AS [27,28,29,30] in the 'ion root' regime. Agreement has also been obtained in plasmas with net toroidal current and significant magnetic shear in W7-AS [31], and qualitative agreement has been reported in TJ-II [32].…”
Section: Neoclassical Transport In Stellarators: Theory and Experimentssupporting
confidence: 82%
“…with exponential decay towards the center of the plasma. This choice is supported by W7-AS results [15], where the anomalous heat diffusivity obtained from power balance analysis decreases with increasing n e at the edge.…”
Section: Iib X2 Heating From Lfs In the Equatorial Planementioning
confidence: 66%
“…For this purpose two simulations are carried out. To put the results of the simulation with the ITG model in relation, the first simulation employs for comparison an empirical anomalous transport model which has been obtained from W7-AS where the diffusion coefficient scales with the absorbed power and inversely with the density, a ∼ P 3/4 n −1 [24,25]. For this first simulation the diffusion coefficient has been adjusted to be on the order of 1 m 2 /s at the plasma edge.…”
Section: Plasma Transportmentioning
confidence: 99%