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Resonant magnetic perturbations of edge-plasmas in toroidal confinement devices
TE Evans - Plasma Physics and Controlled Fusion, 2015 - iopscience.iop.org
Controlling the boundary layer in fusion-grade, high-performance, plasma discharges is
essential for the successful development of toroidal magnetic confinement power generating …
essential for the successful development of toroidal magnetic confinement power generating …
Steady-state tokamak research: core physics
M Kikuchi, M Azumi - Reviews of Modern Physics, 2012 - APS
Tokamaks have demonstrated excellent plasma confinement capability because of their
symmetry but has an intrinsic drawback because of their pulsed inductive operation. Efforts …
symmetry but has an intrinsic drawback because of their pulsed inductive operation. Efforts …
First Observation of Edge Localized Modes Mitigation with Resonant and Nonresonant<? format?> Magnetic Perturbations in ASDEX Upgrade
First experiments with nonaxisymmetric magnetic perturbations, toroidal mode number n= 2,
produced by newly installed in-vessel saddle coils in the ASDEX Upgrade tokamak show …
produced by newly installed in-vessel saddle coils in the ASDEX Upgrade tokamak show …
Edge stability and transport control with resonant magnetic perturbations in collisionless tokamak plasmas
A critical issue for fusion-plasma research is the erosion of the first wall of the experimental
device due to impulsive heating from repetitive edge magneto-hydrodynamic instabilities …
device due to impulsive heating from repetitive edge magneto-hydrodynamic instabilities …
RMP ELM suppression in DIII-D plasmas with ITER similar shapes and collisionalities
Large Type-I edge localized modes (ELMs) are completely eliminated with small n= 3
resonant magnetic perturbations (RMP) in low average triangularity,, plasmas and in ITER …
resonant magnetic perturbations (RMP) in low average triangularity,, plasmas and in ITER …
ELM control strategies and tools: status and potential for ITER
Operating ITER in the reference inductive scenario at the design values of I p= 15 MA and Q
DT= 10 requires the achievement of good H-mode confinement that relies on the presence …
DT= 10 requires the achievement of good H-mode confinement that relies on the presence …
Survey of the H-mode power threshold and transition physics studies in ASDEX Upgrade
F Ryter, SK Rathgeber, LB Orte, M Bernert… - Nuclear …, 2013 - iopscience.iop.org
An overview of the H-mode threshold power in ASDEX Upgrade which addresses the impact
of the tungsten versus graphite wall, the dependences upon plasma current and density, as …
of the tungsten versus graphite wall, the dependences upon plasma current and density, as …
Material testing facilities and programs for plasma-facing component testing
Component development for operation in a large-scale fusion device requires thorough
testing and qualification for the intended operational conditions. In particular environments …
testing and qualification for the intended operational conditions. In particular environments …
Calculations of two-fluid linear response to non-axisymmetric fields in tokamaks
NM Ferraro - Physics of Plasmas, 2012 - pubs.aip.org
The zero-frequency linear plasma response to static applied non-axisymmetric fields is
calculated using a resistive two-fluid model in diverted, toroidal geometry. Within this model …
calculated using a resistive two-fluid model in diverted, toroidal geometry. Within this model …
Tungsten as first wall material in fusion devices
M Kaufmann, R Neu - Fusion Engineering and Design, 2007 - Elsevier
The observation in JET of co-deposition of tritium with carbon has led to a broad discussion
on the replacement of graphite by a high-Z material for the first wall coverage. Moreover, due …
on the replacement of graphite by a high-Z material for the first wall coverage. Moreover, due …