Predicting and Optimizing Pedestal Structure with the EPED Model

POSTER

Abstract

The pressure and temperature at the top of the edge transport barrier ("pedestal height"), play a strong role in fusion performance, with fusion power density in power plant scale plasmas scaling roughly with the square of the pedestal pressure. The EPED model [1] was developed to predict the structure of the pedestal based on two calculated constraints (1) onset of stiff transport due to nearly-local kinetic ballooning modes (KBM), and (2) global constraint on the pedestal height due to peeling-ballooning (P-B) modes. Recent developments have included generalization of the KBM constraint, and coupling of EPED to SOLPS, which enables self-consistent determination of sources and introduction of non-stiff transport constraints into EPED. EPED has been used to predict the Super H Mode regime and to guide record-setting experiments on DIII-D and C-Mod exploring this regime. Here we present recent work on updates to the EPED model, coupling of the model to core and SOL models, and validation of the model in a wide variety of experimental conditions, including in Super H-Mode experiments.

Publication: [1] P.B. Snyder et al, Nucl. Fusion 51, 103016 (2011); Phys. Plasmas 16 056118 (2009).
[2] J.F. Parisi et al, arXiv:2312.05216 (2023), arXiv:2401.14260 (2024).
[3] W.M. Solomon et al., PRL 113 135001 (2014); P.B. Snyder et al. Nucl Fusion 55 083026 (2015).
[4] Hughes, J.W. et al., Nucl. Fus. 58 112003 (2018). Snyder, P.B. et al., Nucl. Fus. 59 086017 (2019).
[5] Knolker, M. et al., PoP 27 102506 (2020); T.M. Wilks et al., Nucl. Fusion 61 126064 (2021).

Presenters

  • Philip B Snyder

    Oak Ridge National Lab

Authors

  • Philip B Snyder

    Oak Ridge National Lab

  • Jin Myung Park

    Oak Ridge National Laboratory

  • Howard R Wilson

    Oak Ridge National Laboratory

  • Cami S Collins

    Oak Ridge National Lab

  • Ehab M Hassan

    Oak Ridge National Laboratory

  • Jerry W Hughes

    MIT Plasma Science and Fusion Center, Massachusetts Institute of Technology

  • Matthias Knolker

    General Atomics

  • Tom H Osborne

    General Atomics - San Diego, General Atomics

  • Jason F Parisi

    Princeton Plasma Physics Laboratory, Princeton University, Princeton Plasma Physics Laboratory

  • Morgan W Shafer

    Oak Ridge National Laboratory

  • Wayne M Solomon

    General Atomics

  • Robert S Wilcox

    Oak Ridge National Laboratory

  • Theresa M Wilks

    MIT Plasma Science and Fusion Center, MIT-PSFC