2017
DOI: 10.1088/1741-4326/aa7691
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3D effects on transport and plasma control in the TJ-II stellarator

Abstract: The effects of 3D geometry are explored in TJ-II from two relevant points of view: neoclassical transport and modification of stability and dispersion relation of waves. Particle fuelling and impurity transport are studied considering the 3D transport properties, paying attention to both neoclassical transport and other possible mechanisms. The effects of the 3D magnetic topology on stability, confinement and Alfvén Eigenmodes properties are also explored, showing the possibility of controlling Alfvén modes by… Show more

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Cited by 19 publications
(15 citation statements)
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References 51 publications
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“…The results show that the heating scenario (ECRH vs NBI) induces a change in the wavenumber spectra. Turbulence level is higher in ECRH than in NBI plasmas, which is in agreement with previous results obtained in the TJ-II stellarator [190]. The variations in the isotope mass ratio do not induce changes in the properties of the turbulence, as seen in figure 3.28.…”
Section: Influence Of Isotope Mass On Plasma Turbulencesupporting
confidence: 91%
“…The results show that the heating scenario (ECRH vs NBI) induces a change in the wavenumber spectra. Turbulence level is higher in ECRH than in NBI plasmas, which is in agreement with previous results obtained in the TJ-II stellarator [190]. The variations in the isotope mass ratio do not induce changes in the properties of the turbulence, as seen in figure 3.28.…”
Section: Influence Of Isotope Mass On Plasma Turbulencesupporting
confidence: 91%
“…A non-axisymmetric E × B shear inducing toroidally localized turbulence with an applied magnetic perturbation field in EAST plasma confinement [13][14][15]. Understanding the 3D interaction between the turbulence and E × B shear is thus the key to uncovering the physics behind the ELM control.…”
Section: Nuclear Fusionmentioning
confidence: 99%
“…The TJ-II is a four-period, low magnetic shear (Δι ≤ 6 %) stellarator located at CIEMAT, Madrid, Spain [44]. Its major radius, R0, is 1.5 m, and its average minor radius, a0, is ≤ 0.22 m. A set of poloidal, toroidal and vertical coils creates its fully 3-dimensional magnetic-field with bean shaped cross-section, central magnetic field, B(0) ≤ 1.1 T, and total plasma volume of around 1.1 m 3 .…”
Section: Tj-iimentioning
confidence: 99%