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Title: Microturbulence in DIII-D tokamak pedestal. III. Effects of collisions

Abstract

Gyrokinetic simulations of the H-mode pedestal in DIII-D discharge 145701 find that the kinetic ballooning mode (KBM) is the most unstable mode for low toroidal numbers (n ≤ 25) and that the trapped electron mode (TEM) dominates over the KBM at higher toroidal mode numbers for realistic pressure gradients in the pedestal. Collisions reduce the TEM growth rate but have little effects on the KBM. KBM has the conventional ballooning mode structure peaking at the outer mid-plane, while TEM has an unconventional mode structure peaking at the top and bottom of the poloidal plane.

Authors:
ORCiD logo [1]; ORCiD logo [2];  [2];  [3];  [1];  [4]
  1. Peking Univ., Beijing (China)
  2. Univ. of California, Irvine, CA (United States)
  3. Zhejiang Univ., Hangzhou (China).
  4. General Atomics, San Diego, CA (United States)
Publication Date:
Research Org.:
Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States). Oak Ridge Leadership Computing Facility (OLCF); Lawrence Berkeley National Lab. (LBNL), Berkeley, CA (United States)
Sponsoring Org.:
USDOE Office of Science (SC)
OSTI Identifier:
1497077
Grant/Contract Number:  
AC02-05CH11231; AC05-00OR22725; SC0010416
Resource Type:
Accepted Manuscript
Journal Name:
Physics of Plasmas
Additional Journal Information:
Journal Volume: 23; Journal Issue: 12; 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

Citation Formats

Liao, X., Lin, Z., Holod, I., Xiao, Y., Li, B., and Snyder, P. B. Microturbulence in DIII-D tokamak pedestal. III. Effects of collisions. United States: N. p., 2016. Web. doi:10.1063/1.4972079.
Liao, X., Lin, Z., Holod, I., Xiao, Y., Li, B., & Snyder, P. B. Microturbulence in DIII-D tokamak pedestal. III. Effects of collisions. United States. https://doi.org/10.1063/1.4972079
Liao, X., Lin, Z., Holod, I., Xiao, Y., Li, B., and Snyder, P. B. Fri . "Microturbulence in DIII-D tokamak pedestal. III. Effects of collisions". United States. https://doi.org/10.1063/1.4972079. https://www.osti.gov/servlets/purl/1497077.
@article{osti_1497077,
title = {Microturbulence in DIII-D tokamak pedestal. III. Effects of collisions},
author = {Liao, X. and Lin, Z. and Holod, I. and Xiao, Y. and Li, B. and Snyder, P. B.},
abstractNote = {Gyrokinetic simulations of the H-mode pedestal in DIII-D discharge 145701 find that the kinetic ballooning mode (KBM) is the most unstable mode for low toroidal numbers (n ≤ 25) and that the trapped electron mode (TEM) dominates over the KBM at higher toroidal mode numbers for realistic pressure gradients in the pedestal. Collisions reduce the TEM growth rate but have little effects on the KBM. KBM has the conventional ballooning mode structure peaking at the outer mid-plane, while TEM has an unconventional mode structure peaking at the top and bottom of the poloidal plane.},
doi = {10.1063/1.4972079},
journal = {Physics of Plasmas},
number = 12,
volume = 23,
place = {United States},
year = {Fri Dec 16 00:00:00 EST 2016},
month = {Fri Dec 16 00:00:00 EST 2016}
}

Journal Article:
Free Publicly Available Full Text
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Citation Metrics:
Cited by: 4 works
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Figures / Tables:

Figure 1 Figure 1: Plasma profiles in the pedestal region of DIII-D discharge 145701 at time 33 ms as functions of normalized poloidal flux (${\psi}_n$). The panels, from left to right, show normalized temperatures (Ti and Te), and density (ni = ne) profiles, inverse temperature and density scale length, be values, andmore » safety factor (q). The vertical black dashed line indicates the radial position of the peak gradient region of pedestal and ${\beta}_e$ = 0.14% at the dotted line position.« less

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Figures/Tables have been extracted from DOE-funded journal article accepted manuscripts.