NSTX-U Supported by Culham Sci Ctr York U Chubu U Fukui U Hiroshima U Hyogo U Kyoto U Kyushu U Kyushu Tokai U NIFS Niigata U U Tokyo JAEA Inst for Nucl.

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Presentation transcript:

NSTX-U Supported by Culham Sci Ctr York U Chubu U Fukui U Hiroshima U Hyogo U Kyoto U Kyushu U Kyushu Tokai U NIFS Niigata U U Tokyo JAEA Inst for Nucl Res, Kiev Ioffe Inst TRINITI Chonbuk Natl U NFRI KAIST POSTECH Seoul Natl U ASIPP CIEMAT FOM Inst DIFFER ENEA, Frascati CEA, Cadarache IPP, Jülich IPP, Garching ASCR, Czech Rep Coll of Wm & Mary Columbia U CompX General Atomics FIU INL Johns Hopkins U LANL LLNL Lodestar MIT Lehigh U Nova Photonics ORNL PPPL Princeton U Purdue U SNL Think Tank, Inc. UC Davis UC Irvine UCLA UCSD U Colorado U Illinois U Maryland U Rochester U Tennessee U Tulsa U Washington U Wisconsin X Science LLC NSTX-U Supported by JRT15 J.W. Berkery 1, S.A. Sabbagh 1, J.-K. Park 2 1 Columbia U., 2 PPPL PPPL December 6, 2013

JRT15 Meeting, December 6 th, 2103 (J.W. Berkery) NSTX 2 “Broadened pressure profiles generally improve global stability” NSTX disruptivity NSTX-U projected ideal stability

JRT15 Meeting, December 6 th, 2103 (J.W. Berkery) NSTX 3 Focus on: details of plasma at pressure peaking / current peaking/broadening disruptive limits, and how to avoid such limits (previous slide) the impact of broadened current and pressure profiles on stability in plasmas that are close to being fully non-inductive pressure peaking / current profile data in light of a plasma under active MHD control how these zeroth order parameters can be influenced by more modern hypotheses – e.g. kinetic stabilization different dependencies not explicitly stated in the JRT15: the effect of rotation, q, anisotropic EP distribution… MS TSG suggestions for the direction of the JRT15

JRT15 Meeting, December 6 th, 2103 (J.W. Berkery) NSTX 4 Pressure profile effects kinetic stability by changing the location of mode-particle resonances Example: ITER case with ITB: Strong internal gradients create large ω * —Cause difference between ω φ and ω EXB. —Enables resonance with precession drift of trapped thermal ions if ω φ is low. Strong gradients dashed lines = “standard” ITER advanced scenario

JRT15 Meeting, December 6 th, 2103 (J.W. Berkery) NSTX 5 “Validate theoretical models of… global stability response to varied heating and current drive deposition” Anisotropy of EPs can effect stability and we plan to study this in NSTX-U injection pitch χ 0 ~NSTX Contours of γτ w with isotropic thermal particles + anisotropic EPs: fluid correction and δW K spread δχ 0 Fluid + Kinetic Effects

JRT15 Meeting, December 6 th, 2103 (J.W. Berkery) NSTX 6 Study of classical and neoclassical tearing mode stability vs. pressure gradient and q-shear Classical and neoclassical tearing modes can be more important in NSTX-U, despite the favorable Glasser and curvature effects, due to high pressure and bootstrap current fraction Study on classical tearing mode –Can be destabilized by both pressure and current broadening –Resistive DCON can be used to more precisely estimate classical tearing mode index △ ′ and can be compared with experiments Neoclassical tearing mode (NTM) –In low aspect ratio, neoclassical and resistive interchange effects can be comparable –Depending on (p′/q′) and (p′/q′) 2, respectively, and thus can be further destabilized if current broadening leads to q-shear reduction Study can be extended onto rotational-shear stabilization as shown in NSTX

JRT15 Meeting, December 6 th, 2103 (J.W. Berkery) NSTX 7 xxx

JRT15 Meeting, December 6 th, 2103 (J.W. Berkery) NSTX 8 Conduct experiments and analysis to quantify the impact of broadened current and pressure profiles on tokamak plasma confinement and stability. Broadened pressure profiles generally improve global stability but can also affect transport and confinement, while broadened current profiles can have both beneficial and adverse impacts on confinement and stability. This research will examine a variety of heating and current drive techniques in order to validate theoretical models of both the actuator performance and the transport and global stability response to varied heating and current drive deposition. JRT15