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

Title: Toroidal modeling of runaway electron loss due to 3-D fields in DIII-D and COMPASS

Abstract

The 3-D field induced relativistic runaway electron (RE) loss has been simulated for DIII-D, COMPASS and ITER plasmas, utilizing the MARS-F code incorporated with the recently developed and updated RE orbit module (REORBIT). Modeling shows effectively 100% loss of a post-disruption, high-current runaway beam in DIII-D, due to the 1 kG level of magnetic field perturbation produced by a fast growing n = 1 resistive kink instability. The RE loss is shown to be independent of the particle energy or the initial location of particles in the configuration space. Applied resonant magnetic perturbation (RMP) fields from in-vessel coils are not effective for RE beam mitigation in DIII-D, but do produce finite (>10%) RE loss in COMPASS, consistent with experimental observations in above two devices. The major reasons for this difference in RE control by RMP between these two devices are (i) the coil proximity to the RE beam and (ii) the effective coil current scaling versus the machine size and the toroidal magnetic field. About 10% RE loss fraction is also predicted for an ITER 15 MA scenario with pre-disruption plasma, highlighting the role of the plasma response. Up to 30% loss is computed, however, by artificially scaling the equilibriummore » pressure to zero. This is due to the more resistive plasma response and stronger resulting field line stochasticity. Distributions of the lost REs to the limiting surface show poloidally peaked profile near the high-field-side in both DIII-D and COMPASS, covering about 100o poloidal angle. Higher perturbation field level and/or higher particle energy also result in REs being lost to the low-field-side of the limiting surface of these two devices, increasing the effective wetted area. Finally, for the modeled ITER plasmas, the applied RMP field, with optimal poloidal spectrum that maximizes the edge localized mode control, leads to REs being lost to the lower divertor region of the limiting surface within a narrow poloidal band.« less

Authors:
ORCiD logo [1]; ORCiD logo [1]; ORCiD logo [2];  [3];  [4]; ORCiD logo [1];  [5]; ORCiD logo [1];  [6]
  1. General Atomics, San Diego, CA (United States)
  2. Institute of Plasma Physics of the CAS, Prague (Czechia); Charles Univ., Prague (Czech Republic)
  3. Institute of Plasma Physics of the CAS, Prague (Czechia)
  4. Institute of Plasma Physics of the CAS, Prague (Czechia); Czech Technical Univ., Prague (Czech Republic)
  5. 2SLS2 Consulting, San Diego, CA (United States)
  6. Donghua University, Shanghai (China)
Publication Date:
Research Org.:
General Atomics, San Diego, CA (United States)
Sponsoring Org.:
USDOE Office of Science (SC)
OSTI Identifier:
1673624
Alternate Identifier(s):
OSTI ID: 1671157
Grant/Contract Number:  
FG02-95ER54309; SC0016452; FC02-04ER54698; 633053
Resource Type:
Accepted Manuscript
Journal Name:
Physics of Plasmas
Additional Journal Information:
Journal Volume: 27; Journal Issue: 10; Journal ID: ISSN 1070-664X
Publisher:
American Institute of Physics (AIP)
Country of Publication:
United States
Language:
English
Subject:
70 PLASMA PHYSICS AND FUSION TECHNOLOGY; runaway current; 3-D field; RE loss

Citation Formats

Liu, Yueqiang, Paz-Soldan, C., Macusova, E., Markovic, T., Ficker, O., Parks, P. B., Kim, C. C., Lao, L. L., and Li, L. Toroidal modeling of runaway electron loss due to 3-D fields in DIII-D and COMPASS. United States: N. p., 2020. Web. doi:10.1063/5.0021154.
Liu, Yueqiang, Paz-Soldan, C., Macusova, E., Markovic, T., Ficker, O., Parks, P. B., Kim, C. C., Lao, L. L., & Li, L. Toroidal modeling of runaway electron loss due to 3-D fields in DIII-D and COMPASS. United States. https://doi.org/10.1063/5.0021154
Liu, Yueqiang, Paz-Soldan, C., Macusova, E., Markovic, T., Ficker, O., Parks, P. B., Kim, C. C., Lao, L. L., and Li, L. Thu . "Toroidal modeling of runaway electron loss due to 3-D fields in DIII-D and COMPASS". United States. https://doi.org/10.1063/5.0021154. https://www.osti.gov/servlets/purl/1673624.
@article{osti_1673624,
title = {Toroidal modeling of runaway electron loss due to 3-D fields in DIII-D and COMPASS},
author = {Liu, Yueqiang and Paz-Soldan, C. and Macusova, E. and Markovic, T. and Ficker, O. and Parks, P. B. and Kim, C. C. and Lao, L. L. and Li, L.},
abstractNote = {The 3-D field induced relativistic runaway electron (RE) loss has been simulated for DIII-D, COMPASS and ITER plasmas, utilizing the MARS-F code incorporated with the recently developed and updated RE orbit module (REORBIT). Modeling shows effectively 100% loss of a post-disruption, high-current runaway beam in DIII-D, due to the 1 kG level of magnetic field perturbation produced by a fast growing n = 1 resistive kink instability. The RE loss is shown to be independent of the particle energy or the initial location of particles in the configuration space. Applied resonant magnetic perturbation (RMP) fields from in-vessel coils are not effective for RE beam mitigation in DIII-D, but do produce finite (>10%) RE loss in COMPASS, consistent with experimental observations in above two devices. The major reasons for this difference in RE control by RMP between these two devices are (i) the coil proximity to the RE beam and (ii) the effective coil current scaling versus the machine size and the toroidal magnetic field. About 10% RE loss fraction is also predicted for an ITER 15 MA scenario with pre-disruption plasma, highlighting the role of the plasma response. Up to 30% loss is computed, however, by artificially scaling the equilibrium pressure to zero. This is due to the more resistive plasma response and stronger resulting field line stochasticity. Distributions of the lost REs to the limiting surface show poloidally peaked profile near the high-field-side in both DIII-D and COMPASS, covering about 100o poloidal angle. Higher perturbation field level and/or higher particle energy also result in REs being lost to the low-field-side of the limiting surface of these two devices, increasing the effective wetted area. Finally, for the modeled ITER plasmas, the applied RMP field, with optimal poloidal spectrum that maximizes the edge localized mode control, leads to REs being lost to the lower divertor region of the limiting surface within a narrow poloidal band.},
doi = {10.1063/5.0021154},
journal = {Physics of Plasmas},
number = 10,
volume = 27,
place = {United States},
year = {Thu Oct 08 00:00:00 EDT 2020},
month = {Thu Oct 08 00:00:00 EDT 2020}
}

Works referenced in this record:

Recent DIII-D advances in runaway electron measurement and model validation
journal, May 2019


Simulation of runaway electrons, transport affected by J-TEXT resonant magnetic perturbation
journal, July 2016


Loss of relativistic electrons when magnetic surfaces are broken
journal, October 2016

  • Boozer, Allen H.; Punjabi, Alkesh
  • Physics of Plasmas, Vol. 23, Issue 10
  • DOI: 10.1063/1.4966046

Runaway electrons and ITER
journal, March 2017


Destabilization of magnetosonic-whistler waves by a relativistic runaway beam
journal, June 2006

  • Fülöp, T.; Pokol, G.; Helander, P.
  • Physics of Plasmas, Vol. 13, Issue 6
  • DOI: 10.1063/1.2208327

Runaway electron losses caused by resonant magnetic perturbations in ITER
journal, July 2011


Role of Kinetic Instability in Runaway-Electron Avalanches and Elevated Critical Electric Fields
journal, June 2018


Runaway electron beam stability and decay in COMPASS
journal, August 2019


Linear MHD stability analysis of post-disruption plasmas in ITER
journal, May 2016


Numerical analysis of runaway tokamak equilibrium
journal, February 1990


Avalanche runaway growth rate from a momentum-space orbit analysis
journal, June 1999

  • Parks, P. B.; Rosenbluth, M. N.; Putvinski, S. V.
  • Physics of Plasmas, Vol. 6, Issue 6
  • DOI: 10.1063/1.873524

Runaway electron drift orbits in magnetostatic perturbed fields
journal, March 2011


Spatiotemporal Evolution of Runaway Electron Momentum Distributions in Tokamaks
journal, June 2017


Runaway electron mitigation by 3D fields in the ASDEX-Upgrade experiment
journal, November 2017


Measurement of runaway electron energy distribution function during high-Z gas injection into runaway electron plateaus in DIII-Da)
journal, May 2015

  • Hollmann, E. M.; Parks, P. B.; Commaux, N.
  • Physics of Plasmas, Vol. 22, Issue 5
  • DOI: 10.1063/1.4921149

Test particles dynamics in the JOREK 3D non-linear MHD code and application to electron transport in a disruption simulation
journal, December 2017


Kink instabilities of the post-disruption runaway electron beam at low safety factor
journal, March 2019

  • Paz-Soldan, C.; Eidietis, N. W.; Liu, Y. Q.
  • Plasma Physics and Controlled Fusion, Vol. 61, Issue 5
  • DOI: 10.1088/1361-6587/aafd15

Runaway electron transport via tokamak microturbulence
journal, October 2009


Runaway electron confinement modelling for rapid shutdown scenarios in DIII-D, Alcator C-Mod and ITER
journal, May 2011


Theory of runaway electrons in ITER: Equations, important parameters, and implications for mitigation
journal, March 2015


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

Magnetic surface loss and electron runaway
journal, January 2019


MARS-F modeling of post-disruption runaway beam loss by magnetohydrodynamic instabilities in DIII-D
journal, October 2019


Theory for avalanche of runaway electrons in tokamaks
journal, October 1997


First Direct Observation of Runaway-Electron-Driven Whistler Waves in Tokamaks
journal, April 2018


Runaway electron beam dynamics at low plasma density in DIII-D: energy distribution, current profile, and internal instability
journal, January 2020


A backward Monte-Carlo method for time-dependent runaway electron simulations
journal, September 2017

  • Zhang, Guannan; del-Castillo-Negrete, Diego
  • Physics of Plasmas, Vol. 24, Issue 9
  • DOI: 10.1063/1.4986019

Theory of Two Threshold Fields for Relativistic Runaway Electrons
journal, April 2015


Losses of runaway electrons during ergodization
journal, March 2006


Electron acceleration in a JET disruption simulation
journal, August 2018


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

Hamiltonian theory of adiabatic motion of relativistic charged particles
journal, September 2007

  • Tao, Xin; Chan, Anthony A.; Brizard, Alain J.
  • Physics of Plasmas, Vol. 14, Issue 9
  • DOI: 10.1063/1.2773702

Runaway electron experiments at COMPASS in support of the EUROfusion ITER physics research
journal, November 2018

  • Mlynar, J.; Ficker, O.; Macusova, E.
  • Plasma Physics and Controlled Fusion, Vol. 61, Issue 1
  • DOI: 10.1088/1361-6587/aae04a

Chapter 3: MHD stability, operational limits and disruptions
journal, June 2007


Experimental Observation of a Magnetic-Turbulence Threshold for Runaway-Electron Generation in the TEXTOR Tokamak
journal, June 2013