Presentation is loading. Please wait.

Presentation is loading. Please wait.

1 Columbia U Comp-X General Atomics INEL Johns Hopkins U LANL LLNL Lodestar MIT Nova Photonics NYU ORNL PPPL PSI SNL UC Davis UC Irvine UCLA UCSD U Maryland.

Similar presentations


Presentation on theme: "1 Columbia U Comp-X General Atomics INEL Johns Hopkins U LANL LLNL Lodestar MIT Nova Photonics NYU ORNL PPPL PSI SNL UC Davis UC Irvine UCLA UCSD U Maryland."— Presentation transcript:

1 1 Columbia U Comp-X General Atomics INEL Johns Hopkins U LANL LLNL Lodestar MIT Nova Photonics NYU ORNL PPPL PSI SNL UC Davis UC Irvine UCLA UCSD U Maryland U New Mexico U Rochester U Washington U Wisconsin Culham Sci Ctr Hiroshima U HIST Kyushu Tokai U Niigata U Tsukuba U U Tokyo Ioffe Inst TRINITI KBSI KAIST ENEA, Frascati CEA, Cadarache IPP, Jülich IPP, Garching U Quebec E.J. Synakowski PPPL Alcator C-Mod Ideas Forum December 2-3, 2004 Perturbative momentum transport studies through configuration modification

2 2 You have found (LaBombard ‘04): small changes in configuration have a profound effect in the edge, and large changes in core V  Tease apart influence of power and SOL flows on core V  : L-H transition induces a change in SOL and core rotation, but other core profiles change, too Minimize changes in other core profiles: Can a rapid (but small ~ 5 - 10 mm) change in X-point balance be used to induce a V  pulse from the edge into the core without changing confinement regime? Simple idea: change configuration rapidly within a discharge and induce a sudden change in the core flow

3 3 Challenge: make a small change in the balance, keep the confinement regime the same, and meaure the V  propagation time to the core In H mode: aim to keep the ELM type the same (or stay in EDA). Change separatrix balance as rapidly as possible. Use as high a power as required to get into desired regime in the most difficult configuration (USN). Then transit to LSN and balanced configs in separate plasmas Measure change in edge flows Measure V  (r,t) deep in the core. Take multiple reproducible shots to make for averagable data to improve time resolution

4 4 Perform systematic scans in ohmic, EDA, and/or benign ELM regimes Ohmic: choose a few density & I p points: USN to LSN highest priority With ICRF, perform a power scan –In addition to EDA or ELMy H mode, L mode would also be of value Also basic confinement knobs like I p

5 5 (B): isotope swap would provide an additional knob Change edge Mach flow by using hydrogen, induce edge flow perturbations with configuration changes If edge flows increase with H, is there a corresponding increase in core flow velocity? For a given confinement time, how do core and edge rotation speeds differ? Start-of-run, or end-of-run use of H will minimize impact on RF Even a comparison of ohmic current and density scans along the lines of those just described would be of value Other fans of an isotope swap? Turbulence studies, including imaging?


Download ppt "1 Columbia U Comp-X General Atomics INEL Johns Hopkins U LANL LLNL Lodestar MIT Nova Photonics NYU ORNL PPPL PSI SNL UC Davis UC Irvine UCLA UCSD U Maryland."

Similar presentations


Ads by Google