DOE PAGES title logo U.S. Department of Energy
Office of Scientific and Technical Information

Title: Equilibrium drives of the low and high field side n = 2 plasma response and impact on global confinement

Abstract

Abstract. The nature of the multi-modal n=2 plasma response and its impact on global confinement is studied as a function of the axisymmetric equilibrium pressure, edge safety factor, collisionality, and L vs. H-mode conditions. Varying the relative phase (ΔφUL) between upper and lower in-vessel coils demonstrates that different n=2 poloidal spectra preferentially excite different plasma responses. These different plasma response modes are preferentially detected on the tokamak high-field side (HFS) or low-field side (LFS) midplanes, have different radial extents, couple differently to the resonant surfaces, and have variable impacts on edge stability and global confinement. In all equilibrium conditions studied, the observed confinement degradation shares the same ΔφUL dependence as the coupling to the resonant surfaces given by both ideal (IPEC) and resistive (MARS-F) MHD computation. Varying the edge safety factor shifts the equilibrium field-line pitch and thus the ΔφUL dependence of both the global confinement and the n=2 magnetic response. As edge safety factor is varied, modeling finds that the HFS response (but not the LFS response), the resonant surface coupling, and the edge displacements near the X-point all share the same ΔφUL dependence. The LFS response magnitude is strongly sensitive to the core pressure and is insensitive tomore » the collisionality and edge safety factor. This indicates that the LFS measurements are primarily sensitive to a pressure-driven kink-ballooning mode that couples to the core plasma. MHD modeling accurately reproduces these (and indeed all) LFS experimental trends and supports this interpretation. In contrast to the LFS, the HFS magnetic response and correlated global confinement impact is unchanged with plasma pressure, but is strongly reduced in high collisionality conditions in both H and L-mode. This experimentally suggests the bootstrap current drives the HFS response through the kink-peeling mode drive, though surprisingly weak or no dependence on the bootstrap current is seen in modeling. Instead, modeling is revealed to be very sensitive to the details of the edge current profile and equilibrium truncation. Holding truncation fixed, most HFS experimental trends are not captured, thus demonstrating a stark contrast between the robustness of the HFS experimental results and the sensitivity of its computation.« less

Authors:
 [1];  [2];  [2];  [2];  [1];  [1];  [3];  [1];  [4];  [2]
  1. General Atomics, San Diego, CA (United States)
  2. Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States)
  3. General Atomics, San Diego, CA (United States); Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States)
  4. General Atomics, San Diego, CA (United States); Oak Ridge Associated Univ., Oak Ridge, TN (United States)
Publication Date:
Research Org.:
Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States); General Atomics, San Diego, CA (United States)
Sponsoring Org.:
USDOE
Contributing Org.:
Oak Ridge Associated Universities, Oak Ridge, Tennessee 37830, USA Princeton Plasma Physics Laboratory, Princeton, New Jersey 08543, USA
OSTI Identifier:
1254901
Alternate Identifier(s):
OSTI ID: 1245030; OSTI ID: 1369217
Report Number(s):
DOE-GA-54698
Journal ID: ISSN 0029-5515
Grant/Contract Number:  
AC02-09CH11466; AC05-06OR23100; FC02-04ER54698
Resource Type:
Accepted Manuscript
Journal Name:
Nuclear Fusion
Additional Journal Information:
Journal Volume: 56; Journal Issue: 5; Journal ID: ISSN 0029-5515
Publisher:
IOP Science
Country of Publication:
United States
Language:
English
Subject:
70 PLASMA PHYSICS AND FUSION TECHNOLOGY

Citation Formats

Paz-Soldan, C., Logan, N. C., Haskey, S. R., Nazikian, R., Strait, E. J., Chen, X., Ferraro, N. M., King, J. D., Lyons, B. C., and Park, J. -K. Equilibrium drives of the low and high field side n = 2 plasma response and impact on global confinement. United States: N. p., 2016. Web. doi:10.1088/0029-5515/56/5/056001.
Paz-Soldan, C., Logan, N. C., Haskey, S. R., Nazikian, R., Strait, E. J., Chen, X., Ferraro, N. M., King, J. D., Lyons, B. C., & Park, J. -K. Equilibrium drives of the low and high field side n = 2 plasma response and impact on global confinement. United States. https://doi.org/10.1088/0029-5515/56/5/056001
Paz-Soldan, C., Logan, N. C., Haskey, S. R., Nazikian, R., Strait, E. J., Chen, X., Ferraro, N. M., King, J. D., Lyons, B. C., and Park, J. -K. Thu . "Equilibrium drives of the low and high field side n = 2 plasma response and impact on global confinement". United States. https://doi.org/10.1088/0029-5515/56/5/056001. https://www.osti.gov/servlets/purl/1254901.
@article{osti_1254901,
title = {Equilibrium drives of the low and high field side n = 2 plasma response and impact on global confinement},
author = {Paz-Soldan, C. and Logan, N. C. and Haskey, S. R. and Nazikian, R. and Strait, E. J. and Chen, X. and Ferraro, N. M. and King, J. D. and Lyons, B. C. and Park, J. -K.},
abstractNote = {Abstract. The nature of the multi-modal n=2 plasma response and its impact on global confinement is studied as a function of the axisymmetric equilibrium pressure, edge safety factor, collisionality, and L vs. H-mode conditions. Varying the relative phase (ΔφUL) between upper and lower in-vessel coils demonstrates that different n=2 poloidal spectra preferentially excite different plasma responses. These different plasma response modes are preferentially detected on the tokamak high-field side (HFS) or low-field side (LFS) midplanes, have different radial extents, couple differently to the resonant surfaces, and have variable impacts on edge stability and global confinement. In all equilibrium conditions studied, the observed confinement degradation shares the same ΔφUL dependence as the coupling to the resonant surfaces given by both ideal (IPEC) and resistive (MARS-F) MHD computation. Varying the edge safety factor shifts the equilibrium field-line pitch and thus the ΔφUL dependence of both the global confinement and the n=2 magnetic response. As edge safety factor is varied, modeling finds that the HFS response (but not the LFS response), the resonant surface coupling, and the edge displacements near the X-point all share the same ΔφUL dependence. The LFS response magnitude is strongly sensitive to the core pressure and is insensitive to the collisionality and edge safety factor. This indicates that the LFS measurements are primarily sensitive to a pressure-driven kink-ballooning mode that couples to the core plasma. MHD modeling accurately reproduces these (and indeed all) LFS experimental trends and supports this interpretation. In contrast to the LFS, the HFS magnetic response and correlated global confinement impact is unchanged with plasma pressure, but is strongly reduced in high collisionality conditions in both H and L-mode. This experimentally suggests the bootstrap current drives the HFS response through the kink-peeling mode drive, though surprisingly weak or no dependence on the bootstrap current is seen in modeling. Instead, modeling is revealed to be very sensitive to the details of the edge current profile and equilibrium truncation. Holding truncation fixed, most HFS experimental trends are not captured, thus demonstrating a stark contrast between the robustness of the HFS experimental results and the sensitivity of its computation.},
doi = {10.1088/0029-5515/56/5/056001},
journal = {Nuclear Fusion},
number = 5,
volume = 56,
place = {United States},
year = {Thu Mar 31 00:00:00 EDT 2016},
month = {Thu Mar 31 00:00:00 EDT 2016}
}

Journal Article:
Free Publicly Available Full Text
Publisher's Version of Record

Citation Metrics:
Cited by: 30 works
Citation information provided by
Web of Science

Save / Share:

Works referenced in this record:

Computation of three-dimensional tokamak and spherical torus equilibria
journal, May 2007

  • Park, Jong-kyu; Boozer, Allen H.; Glasser, Alan H.
  • Physics of Plasmas, Vol. 14, Issue 5
  • DOI: 10.1063/1.2732170

Dependence of neoclassical toroidal viscosity on the poloidal spectrum of applied nonaxisymmetric fields
journal, February 2016


Experimental tests of linear and nonlinear three-dimensional equilibrium models in DIII-D
journal, July 2015

  • King, J. D.; Strait, E. J.; Lazerson, S. A.
  • Physics of Plasmas, Vol. 22, Issue 7
  • DOI: 10.1063/1.4923017

Measurement and modeling of three-dimensional equilibria in DIII-D
journal, May 2011

  • Lanctot, M. J.; Reimerdes, H.; Garofalo, A. M.
  • Physics of Plasmas, Vol. 18, Issue 5
  • DOI: 10.1063/1.3593009

Experimental imaging of separatrix splitting on DIII-D
journal, November 2012


Three-dimensional equilibria and island energy transport due to resonant magnetic perturbation edge localized mode suppression on DIII-D
journal, November 2015

  • King, J. D.; Strait, E. J.; Nazikian, R.
  • Physics of Plasmas, Vol. 22, Issue 11
  • DOI: 10.1063/1.4935486

Neoclassical conductivity and bootstrap current formulas for general axisymmetric equilibria and arbitrary collisionality regime
journal, July 1999

  • Sauter, O.; Angioni, C.; Lin-Liu, Y. R.
  • Physics of Plasmas, Vol. 6, Issue 7
  • DOI: 10.1063/1.873240

An upgrade of the magnetic diagnostic system of the DIII-D tokamak for non-axisymmetric measurements
journal, August 2014

  • King, J. D.; Strait, E. J.; Boivin, R. L.
  • Review of Scientific Instruments, Vol. 85, Issue 8
  • DOI: 10.1063/1.4891817

Effect of resonant magnetic perturbations on low collisionality discharges in MAST and a comparison with ASDEX Upgrade
journal, March 2015


The spectral basis of optimal error field correction on DIII-D
journal, April 2014


Edge localized modes and the pedestal: A model based on coupled peeling–ballooning modes
journal, May 2002

  • Snyder, P. B.; Wilson, H. R.; Ferron, J. R.
  • Physics of Plasmas, Vol. 9, Issue 5
  • DOI: 10.1063/1.1449463

Advances in the physics understanding of ELM suppression using resonant magnetic perturbations in DIII-D
journal, January 2015


The importance of matched poloidal spectra to error field correction in DIII-D
journal, July 2014

  • Paz-Soldan, C.; Lanctot, M. J.; Logan, N. C.
  • Physics of Plasmas, Vol. 21, Issue 7
  • DOI: 10.1063/1.4886795

Validation of the linear ideal magnetohydrodynamic model of three-dimensional tokamak equilibria
journal, March 2010

  • Lanctot, M. J.; Reimerdes, H.; Garofalo, A. M.
  • Physics of Plasmas, Vol. 17, Issue 3
  • DOI: 10.1063/1.3335237

Understanding edge-localized mode mitigation by resonant magnetic perturbations on MAST
journal, March 2013


Homoclinic tangles, bifurcations and edge stochasticity in diverted tokamaks
journal, April 2004

  • Evans, T. E.; Roeder, R. K. W.; Carter, J. A.
  • Contributions to Plasma Physics, Vol. 44, Issue 13
  • DOI: 10.1002/ctpp.200410034

Effect of resonant and non-resonant magnetic braking on error field tolerance in high beta plasmas
journal, September 2009


Enhanced H-mode pedestals with lithium injection in DIII-D
journal, May 2015


Connection between plasma response and resonant magnetic perturbation (RMP) edge localized mode (ELM) suppression in DIII-D
journal, September 2015


Comparisons of linear and nonlinear plasma response models for non-axisymmetric perturbations
journal, May 2013

  • Turnbull, A. D.; Ferraro, N. M.; Izzo, V. A.
  • Physics of Plasmas, Vol. 20, Issue 5
  • DOI: 10.1063/1.4805087

Sustained suppression of type-I edge-localized modes with dominantly n = 2 magnetic fields in DIII-D
journal, July 2013


Edge localized mode control with an edge resonant magnetic perturbation
journal, May 2005

  • Moyer, R. A.; Evans, T. E.; Osborne, T. H.
  • Physics of Plasmas, Vol. 12, Issue 5
  • DOI: 10.1063/1.1888705

Decoupled recovery of energy and momentum with correction of n   =  2 error fields
journal, July 2015


Impact of plasma response on plasma displacements in DIII-D during application of external 3D perturbations
journal, May 2014


Linear ideal MHD predictions for n = 2 non-axisymmetric magnetic perturbations on DIII-D
journal, February 2014


Feedback stabilization of nonaxisymmetric resistive wall modes in tokamaks. I. Electromagnetic model
journal, September 2000

  • Liu, Y. Q.; Bondeson, A.; Fransson, C. M.
  • Physics of Plasmas, Vol. 7, Issue 9
  • DOI: 10.1063/1.1287744

Measurement of plasma boundary displacement by n = 2 magnetic perturbations using imaging beam emission spectroscopy
journal, November 2012


Observation of a Multimode Plasma Response and its Relationship to Density Pumpout and Edge-Localized Mode Suppression
journal, March 2015


Pedestal Bifurcation and Resonant Field Penetration at the Threshold of Edge-Localized Mode Suppression in the DIII-D Tokamak
journal, March 2015


Chapter 4: Power and particle control
journal, June 2007


Suppression of Large Edge-Localized Modes in High-Confinement DIII-D Plasmas with a Stochastic Magnetic Boundary
journal, June 2004


Suppression of Edge Localized Modes in High-Confinement KSTAR Plasmas by Nonaxisymmetric Magnetic Perturbations
journal, July 2012


First Observation of Edge Localized Modes Mitigation with Resonant and Nonresonant Magnetic Perturbations in ASDEX Upgrade
journal, June 2011


Error Field Amplification and Rotation Damping in Tokamak Plasmas
journal, May 2001


Measurement of the Resistive-Wall-Mode Stability in a Rotating Plasma Using Active MHD Spectroscopy
journal, September 2004


Control of Asymmetric Magnetic Perturbations in Tokamaks
journal, November 2007


Sustained Stabilization of the Resistive-Wall Mode by Plasma Rotation in the DIII-D Tokamak
journal, November 2002


Symmetry-Breaking Induced Transport in the Vicinity of a Magnetic Island
journal, November 2001


Ideal magnetohydrodynamic theory of magnetic fusion systems
journal, July 1982


The CHEASE code for toroidal MHD equilibria
journal, September 1996


Observation of Lobes near the X Point in Resonant Magnetic Perturbation Experiments on MAST
journal, June 2012


Multiresonance Effect in Type-I Edge-Localized Mode Control With Low n Fields on JET
journal, August 2010


MOMCON: A spectral code for obtaining three-dimensional magnetohydrodynamic equilibria
journal, February 1986


Evidence for the Importance of Trapped Particle Resonances for Resistive Wall Mode Stability in High Beta Tokamak Plasmas
journal, May 2011


Effect of Collisionality on Kinetic Stability of the Resistive Wall Mode
journal, February 2011


Three-Dimensional Drift Kinetic Response of High- β Plasmas in the DIII-D Tokamak
journal, April 2015


Symmetry-Breaking Induced Transport in the Vicinity of a Magnetic Island
text, January 2001


Works referencing / citing this record:

Predict-first experimental analysis using automated and integrated magnetohydrodynamic modeling
journal, May 2018

  • Lyons, B. C.; Paz-Soldan, C.; Meneghini, O.
  • Physics of Plasmas, Vol. 25, Issue 5
  • DOI: 10.1063/1.5025838

Modal analysis of the full poloidal structure of the plasma response to n = 2 magnetic perturbations
journal, July 2018

  • Munaretto, S.; Strait, E. J.; Haskey, S. R.
  • Physics of Plasmas, Vol. 25, Issue 7
  • DOI: 10.1063/1.5029381