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Title 299: QH-mode studies as a function of edge rotation
Name:Keith Burrell () Affiliation:General Atomics
Research Area:ELM Control & Pedestal Physics Presentation time: Not requested
Co-Author(s): W.M. Solomon, M.E. Fenstermacher, P. Gohil, C.J. Lasnier,T.H. Osborne, P.B. Snyder
Description: Determine whether the QH-mode can be achieved with balanced or even
some co-injection. Investigate effects of edge rotation on QH-mode
plasmas with emphasis on changes in EHO-induced particle transport.
Experimental Approach/Plan: Start the experiment in QH-mode plasmas similar to 128502. Utilize
RMW feedback to null out the remaining intrinsic error field.
Investigate this QH-mode as rotation is made more and more co.
Important questions are the nature of the EHO and its effect on
particle transport.
Background: During the 2006 and 2007 campaigns, we made significant progress in
producing QH-mode plasmas with reduced counter rotation. This was
achieved by optimizing the plasma shape for peeling-ballooning mode
stability and by reducing the intrinsic error fields. The latter is
the key to preventing locked modes at low toroidal rotation. In
moderate beta QH-mode plasmas, we have seen error field amplification
on the ESLD detectors. This effect indicates that we still do not
have optimal error field correction; however, this effect is also what
is needed to use the RWM feedback system to null out the remaining
intrinsic error fields. Unfortunately, we did not have time to apply this
RWM feedback technique in 2007. We have also seen that the particle
transport due to the EHO decreases as the magnitude of the toroidal
rotation decreases. This leads to higher density and higher pedestal
pressures, which in general are destabilizing to the peeling
ballooning modes. However, using the optimized high-triangularity,
double-null shape provided enough stability margin that we remained in
QH-mode.
Resource Requirements: Reverse Ip. 7 NBI sources
Diagnostic Requirements: --
Analysis Requirements: --
Other Requirements: --