Physics of runaway electrons in tokamaks
BN Breizman, P Aleynikov, EM Hollmann… - Nuclear …, 2019 - iopscience.iop.org
Of all electrons, runaway electrons have long been recognized in the fusion community as a
distinctive population. They now attract special attention as a part of ITER mission …
distinctive population. They now attract special attention as a part of ITER mission …
Edge-localized-modes in tokamaks
AW Leonard - Physics of Plasmas, 2014 - pubs.aip.org
Edge-localized-modes (ELMs) are a ubiquitous feature of H-mode in tokamaks. When
gradients in the H-mode transport barrier grow to exceed the MHD stability limit the ELM …
gradients in the H-mode transport barrier grow to exceed the MHD stability limit the ELM …
Progress on the application of ELM control schemes to ITER scenarios from the non-active phase to DT operation
Progress in the definition of the requirements for edge localized mode (ELM) control and the
application of ELM control methods both for high fusion performance DT operation and non …
application of ELM control methods both for high fusion performance DT operation and non …
Filamentary plasma eruptions and their control on the route to fusion energy
The tokamak is the most advanced approach to fusion and is approaching operation under
power-plant conditions, promising sustainable, low-emission, baseload power to the grid. As …
power-plant conditions, promising sustainable, low-emission, baseload power to the grid. As …
[HTML][HTML] ELM divertor peak energy fluence scaling to ITER with data from JET, MAST and ASDEX upgrade
A newly established scaling of the ELM energy fluence using dedicated data sets from JET
operation with CFC & ILW plasma facing components (PFCs), ASDEX Upgrade (AUG) …
operation with CFC & ILW plasma facing components (PFCs), ASDEX Upgrade (AUG) …
The JOREK non-linear extended MHD code and applications to large-scale instabilities and their control in magnetically confined fusion plasmas
JOREK is a massively parallel fully implicit non-linear extended magneto-hydrodynamic
(MHD) code for realistic tokamak X-point plasmas. It has become a widely used versatile …
(MHD) code for realistic tokamak X-point plasmas. It has become a widely used versatile …
Simulation of plasma turbulence in scrape-off layer conditions: the GBS code, simulation results and code validation
Based on the drift-reduced Braginskii equations, the Global Braginskii Solver, GBS, is able
to model the scrape-off layer (SOL) plasma turbulence in terms of the interplay between the …
to model the scrape-off layer (SOL) plasma turbulence in terms of the interplay between the …
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 …
WEST physics basis
C Bourdelle, JF Artaud, V Basiuk, M Bécoulet… - Nuclear …, 2015 - iopscience.iop.org
Abstract With WEST (Tungsten Environment in Steady State Tokamak)(Bucalossi et al 2014
Fusion Eng. Des. 89 907–12), the Tore Supra facility and team expertise (Dumont et al 2014 …
Fusion Eng. Des. 89 907–12), the Tore Supra facility and team expertise (Dumont et al 2014 …
Non-linear magnetohydrodynamic modeling of plasma response to resonant magnetic perturbations
The interaction of static Resonant Magnetic Perturbations (RMPs) with the plasma flows is
modeled in toroidal geometry, using the non-linear resistive MHD code JOREK, which …
modeled in toroidal geometry, using the non-linear resistive MHD code JOREK, which …