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Title: EDGE2D-EIRENE modelling of near SOL Er: possible impact on the H-mode power threshold

Abstract

Recent EDGE2D-EIRENE simulations of JET plasmas showed a significant difference between radial electric field (Er) profiles across the separatrix in two divertor configurations, with the outer strike point on the horizontal target (HT) and vertical target (VT) (Chankin et al 2016 Nucl. Mater. Energy, doi: 10.1016/j.nme.2016.10.004). Under conditions (input power, plasma density) where the HT plasma went into the H-mode, a large positive Er spike in the near scrape-off layer (SOL) was seen in the code output, leading to a very large E × B shear across the separatrix over a narrow region of a fraction of a cm width. No such Er feature was obtained in the code solution for the VT configuration, where the H-mode power threshold was found to be twice as high as in the HT configuration. It was hypothesised that the large E × B shear across the separatrix in the HT configuration could be responsible for the turbulence suppression leading to an earlier (at lower input power) L–H transition compared to the VT configuration. In the present work these ideas are extended to cover some other experimental observations on the H-mode power threshold variation with parameters which typically are not included in the multi-machinemore » H-mode power threshold scalings, namely: ion mass dependence (isotope H–D–T exchange), dependence on the ion ∇B drift direction, and dependence on the wall material composition (ITER-like wall versus carbon wall in JET). In all these cases EDGE2D-EIRENE modelling shows larger positive Er spikes in the near SOL under conditions where the H-mode power threshold is lower, at least in the HT configuration.« less

Authors:
 [1]; ORCiD logo [2];  [3];  [3];  [3];  [3]
  1. Max Planck Institute for Plasma Physics, Garching bei Munchen (Germany)
  2. Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)
  3. Culham Science Centre, Abingdon (United Kingdom). Culham Centre for Fusion Energy (CCFE)
Publication Date:
Research Org.:
Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)
Sponsoring Org.:
USDOE
Contributing Org.:
EUROfusion Consortium, JET, Culham Science Centre, Abingdon (United Kingdom)
OSTI Identifier:
1822099
Grant/Contract Number:  
AC05-00OR22725
Resource Type:
Accepted Manuscript
Journal Name:
Plasma Physics and Controlled Fusion
Additional Journal Information:
Journal Volume: 59; Journal Issue: 4; Journal ID: ISSN 0741-3335
Publisher:
IOP Science
Country of Publication:
United States
Language:
English
Subject:
70 PLASMA PHYSICS AND FUSION TECHNOLOGY

Citation Formats

Chankin, A. V., Delabie, E., Corrigan, G., Harting, D., Maggi, C. F., and Meyer, H. EDGE2D-EIRENE modelling of near SOL Er: possible impact on the H-mode power threshold. United States: N. p., 2017. Web. doi:10.1088/1361-6587/aa5ecc.
Chankin, A. V., Delabie, E., Corrigan, G., Harting, D., Maggi, C. F., & Meyer, H. EDGE2D-EIRENE modelling of near SOL Er: possible impact on the H-mode power threshold. United States. https://doi.org/10.1088/1361-6587/aa5ecc
Chankin, A. V., Delabie, E., Corrigan, G., Harting, D., Maggi, C. F., and Meyer, H. Thu . "EDGE2D-EIRENE modelling of near SOL Er: possible impact on the H-mode power threshold". United States. https://doi.org/10.1088/1361-6587/aa5ecc. https://www.osti.gov/servlets/purl/1822099.
@article{osti_1822099,
title = {EDGE2D-EIRENE modelling of near SOL Er: possible impact on the H-mode power threshold},
author = {Chankin, A. V. and Delabie, E. and Corrigan, G. and Harting, D. and Maggi, C. F. and Meyer, H.},
abstractNote = {Recent EDGE2D-EIRENE simulations of JET plasmas showed a significant difference between radial electric field (Er) profiles across the separatrix in two divertor configurations, with the outer strike point on the horizontal target (HT) and vertical target (VT) (Chankin et al 2016 Nucl. Mater. Energy, doi: 10.1016/j.nme.2016.10.004). Under conditions (input power, plasma density) where the HT plasma went into the H-mode, a large positive Er spike in the near scrape-off layer (SOL) was seen in the code output, leading to a very large E × B shear across the separatrix over a narrow region of a fraction of a cm width. No such Er feature was obtained in the code solution for the VT configuration, where the H-mode power threshold was found to be twice as high as in the HT configuration. It was hypothesised that the large E × B shear across the separatrix in the HT configuration could be responsible for the turbulence suppression leading to an earlier (at lower input power) L–H transition compared to the VT configuration. In the present work these ideas are extended to cover some other experimental observations on the H-mode power threshold variation with parameters which typically are not included in the multi-machine H-mode power threshold scalings, namely: ion mass dependence (isotope H–D–T exchange), dependence on the ion ∇B drift direction, and dependence on the wall material composition (ITER-like wall versus carbon wall in JET). In all these cases EDGE2D-EIRENE modelling shows larger positive Er spikes in the near SOL under conditions where the H-mode power threshold is lower, at least in the HT configuration.},
doi = {10.1088/1361-6587/aa5ecc},
journal = {Plasma Physics and Controlled Fusion},
number = 4,
volume = 59,
place = {United States},
year = {Thu Mar 09 00:00:00 EST 2017},
month = {Thu Mar 09 00:00:00 EST 2017}
}

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Works referencing / citing this record:

A reduced model of neutral-plasma interactions in the edge and scrape-off-layer: Verification comparisons with kinetic Monte Carlo simulations
journal, February 2019

  • Russell, D. A.; Myra, J. R.; Stotler, D. P.
  • Physics of Plasmas, Vol. 26, Issue 2
  • DOI: 10.1063/1.5081670

Dynamics of neon ions after neon gas seeding into tokamak plasma
journal, September 2019


EDGE2D-EIRENE simulations of the influence of isotope effects and anomalous transport coefficients on near scrape-off layer radial electric field
journal, May 2019

  • Chankin, A. V.; Corrigan, G.; Maggi, C. F.
  • Plasma Physics and Controlled Fusion, Vol. 61, Issue 7
  • DOI: 10.1088/1361-6587/ab1629