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Title: Validation of the model for ELM suppression with 3D magnetic fields using low torque ITER baseline scenario discharges in DIII-D

Journal Article · · Physics of Plasmas
DOI:https://doi.org/10.1063/1.5000276· OSTI ID:1398392
 [1];  [2];  [3];  [1];  [4];  [3];  [5];  [6];  [7];  [2];  [8];  [2];  [2];  [2];  [9];  [2];  [10];  [2];  [2];  [11] more »;  [2];  [8];  [7];  [12] « less
  1. Univ. of California, San Diego, La Jolla, CA (United States)
  2. General Atomics, San Diego, CA (United States)
  3. Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States)
  4. General Atomics, San Diego, CA (United States); Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States)
  5. Ludwigs Maximilians Univ., Munchen (Germany)
  6. Oak Ridge Inst. for Science and Education (ORISE), Oak Ridge, TN (United States); General Atomics, San Diego, CA (United States)
  7. Univ. of Wisconsin-Madison, Madison, WI (United States)
  8. Univ. of California, Los Angeles, CA (United States)
  9. Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)
  10. Columbia Univ., New York, NY (United States)
  11. The College of William and Mary, Williamsburg, VA (United States)
  12. Oak Ridge Inst. for Science and Education (ORISE), Oak Ridge, TN (United States); Univ. of California, Los Angeles, CA (United States)

Experiments have been executed in the DIII-D tokamak to extend suppression of Edge Localized Modes (ELMs) with Resonant Magnetic Perturbations (RMPs) to ITER-relevant levels of beam torque. Additionally, the results support the hypothesis for RMP ELM suppression based on transition from an ideal screened response to a tearing response at a resonant surface that prevents expansion of the pedestal to an unstable width [Snyder et al., Nucl. Fusion 51, 103016 (2011) and Wade et al., Nucl. Fusion 55, 023002 (2015)]. In ITER baseline plasmas with I/aB = 1.4 and pedestal ν * ~ 0.15, ELMs are readily suppressed with co- I p neutral beam injection. However, reducing the beam torque from 5 Nm to ≤ 3.5 Nm results in loss of ELM suppression and a shift in the zero-crossing of the electron perpendicular rotation ω e ~ 0 deeper into the plasma. The change in radius of ω e ~ 0 is due primarily to changes to the electron diamagnetic rotation frequency ω e * . Linear plasma response modeling with the resistive MHD code m3d-c1 indicates that the tearing response location tracks the inward shift in ω e ~ 0. At pedestal ν * ~ 1, ELM suppression is also lost when the beam torque is reduced, but the ω e change is dominated by collapse of the toroidal rotation v T . The hypothesis predicts that it should be possible to obtain ELM suppression at reduced beam torque by also reducing the height and width of the ω e * profile. This prediction has been confirmed experimentally with RMP ELM suppression at 0 Nm of beam torque and plasma normalized pressure β N ~ 0.7. This opens the possibility of accessing ELM suppression in low torque ITER baseline plasmas by establishing suppression at low beta and then increasing beta while relying on the strong RMP-island coupling to maintain suppression.

Research Organization:
General Atomics, San Diego, CA (United States); Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)
Sponsoring Organization:
USDOE Office of Science (SC), Fusion Energy Sciences (FES)
Contributing Organization:
DIII-D Team
Grant/Contract Number:
FC02-04ER54698; AC02-76CH03073; AC05-06OR23100; AC52-07NA27344; FG02-04ER54761; FG02-07ER54917; FG02-08ER54984; FG02-08ER54999; FG02ER54809; SC0007880; FG02- 07ER54917; FG02-05ER54809
OSTI ID:
1398392
Alternate ID(s):
OSTI ID: 1392144; OSTI ID: 1839874
Report Number(s):
LLNL-JRNL-752165
Journal Information:
Physics of Plasmas, Vol. 24, Issue 10; ISSN 1070-664X
Publisher:
American Institute of Physics (AIP)Copyright Statement
Country of Publication:
United States
Language:
English
Citation Metrics:
Cited by: 37 works
Citation information provided by
Web of Science

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Cited By (18)

Predict-first experimental analysis using automated and integrated magnetohydrodynamic modeling journal May 2018
Imaging divertor strike point splitting in RMP ELM suppression experiments in the DIII-D tokamak journal October 2018
Two-fluid nonlinear theory of response of tokamak plasma to resonant magnetic perturbation journal November 2018
Main-ion intrinsic toroidal rotation across the ITG/TEM boundary in DIII-D discharges during ohmic and electron cyclotron heating journal April 2019
Penetration properties of resonant magnetic perturbation in EAST Tokamak journal November 2019
Toroidal plasma response based ELM control coil design for EU DEMO journal June 2018
Experimental conditions to suppress edge localised modes by magnetic perturbations in the ASDEX Upgrade tokamak journal July 2018
Grassy-ELM regime with edge resonant magnetic perturbations in fully noninductive plasmas in the DIII-D tokamak journal July 2018
Effects of RMP-induced changes of radial electric fields on microturbulence in DIII-D pedestal top journal February 2019
DIII-D research towards establishing the scientific basis for future fusion reactors journal June 2019
The effect of plasma shape and neutral beam mix on the rotation threshold for RMP-ELM suppression journal March 2019
Tamed stability and transport using controlled non-axisymmetric fields in KSTAR journal March 2019
Direct evidence of E × B flow changes at the onset of resonant magnetic perturbation-driven edge-localized mode crash suppression journal May 2019
Resistive versus ideal plasma response to RMP fields in DIII-D: roles of q 95 and X-point geometry journal June 2019
Optimizing multi-modal, non-axisymmetric plasma response metrics with additional coil rows on DIII-D journal July 2019
Predicting the rotation profile in ITER journal January 2020
Experimental conditions to suppress edge localised modes by magnetic perturbations in the ASDEX Upgrade tokamak text January 2018
Two-Fluid Nonlinear Theory of Response of Tokamak Plasma to Resonant Magnetic Perturbation text January 2018