61st Annual Meeting of the APS Division of Plasma Physics
Volume 64, Number 11
Monday–Friday, October 21–25, 2019;
Fort Lauderdale, Florida
Session AR1: Review: Integrating Core Burning Plasma Performance with Edge Stability for ITER
8:00 AM–9:00 AM,
Monday, October 21, 2019
Room: Floridian Ballroom A-D
Chair: Michael Brown, Swarthmore College
Abstract ID: BAPS.2019.DPP.AR1.1
Abstract: AR1.00001 : \textbf{Understanding the MHD challenges for ITER Q}$=$\textbf{10 operation at reactor relevant conditions}.*
8:00 AM–9:00 AM
Preview Abstract
Author:
Andrea Garofalo
(General Atomics)
DIII-D experiments to assess options for Q$=$10 operation in ITER without
harmful core MHD nor ELMs have advanced both achieved parameters and
understanding of present limitations. Q\textasciitilde 10 performance is
achieved in low collisionality ($\nu $*) ELM-stable plasmas with small co-Ip
NBI torque using RMP ELM suppression, and small counter-Ip NBI torque using
QH-mode edge. Both ELM control approaches are limited by core instabilities,
while the edge regime is strongly affected by local edge torque density. A
rotation threshold for RMP ELM suppression corresponds to a critical radius
for the ExB rotation zero-crossing, and this threshold can be crossed at
widely varying net NBI torques. An ITER-relevant net NBI torque on DIII-D
tends to produce a less ITER-relevant negative local edge torque density,
with severe penalty for ELM suppression. In the QH-mode approach, negative
edge torque density correlates with increased edge ExB shear obtained at low
density, leading to improved confinement at low net NBI torque, and
Q\textgreater 10 equivalent performance at q$_{\mathrm{95}}$\textasciitilde
3. However, low $\nu $* and low q lead to pressure peaking instabilities.
The character of edge fluctuations in QH-mode is key to simultaneous low
torque and low q$_{\mathrm{95}}$ operation: broadband fluctuations are
compatible with low rotation, while a coherent edge harmonic oscillation
(EHO) tends to lock to the wall. A recent discovery is that the plasma-wall
separation gap controls the character of the edge fluctuations: smaller gap
leads to higher-n EHO at low NBI torque; even smaller gap leads to broadband
fluctuations. Too small an outer gap brings back ELMs, with the threshold
gap depending on NBI energy, likely through a gyro-radius dependence of
fast-ion-wall interactions. A large RF-heating fraction could overcome
present limitations by reducing negative edge-torque density, wall
interactions, and pressure peaking from strong core fueling.
*Supported by the US DOE under DE-FC02-04ER54698
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2019.DPP.AR1.1