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Inter-ELM evolution of the edge current density in JET-ILW type i ELMy H-mode plasmas

*Corresponding author for this work
    • University of York
    • Culham Science Centre
    • KTH Royal Institute of Technology
    • Max-Planck-Institut für Plasmaphysik (IPP)
    • Forschungszentrum Jülich GmbH (FZJ)
    • Institute for Plasma Research
    • Universidade de Lisboa
    • Queen's University Belfast
    • University of Helsinki
    • Commissariat a l'Energie Atomique et aux Energies Alternatives (CEA)
    • National Institutes for Quantum Science and Technology (QST)
    • University of Naples Federico II
    • National University of Distance Education
    • National Research Council (CNR)
    • ITER Organization
    • Petersburg Nuclear Physics Institute
    • Parthenope University of Naples
    • National Agency for New Technologies, Energy and Sustainable Economic Development (ENEA)
    • Troitsk Institute for Innovation and Fusion Research
    • Uppsala University
    • National Institute for Cryogenics and Isotopic Technology
    • University of Catania
    • Fusion for Energy (F4E)
    • Aalto University
    • Seoul National University
    • Institute of Plasma Physics (ASIPP CAS)
    • Chalmers University of Technology

    Research output: Contribution to journalArticleScientificpeer-review

    Abstract

    Recent studies (Maggi et al 2015 Nucl. Fusion 55 113031; Maggi et al 2017 Nucl. Fusion 57 116012) have shown that on JET with the Be/W ITER-like wall (JET-ILW) in high β discharges with high D2 gas rates, the inter-ELM temperature pedestal growth is saturated half way through the ELM cycle, leading to plasmas with reduced confinement, and that the linear MHD stability of these pedestals is inconsistent with the peeling-ballooning paradigm (Snyder et al 2002 Phys. Plasmas 9 2037-43; Wilson et al 2002 Phys. Plasmas 9 1277-86). In this paper, the inter-ELM evolution of the edge current density is investigated in a wide range of type I ELMy H-modes on JET-ILW. It is found that in discharges at a low gas rate, the peak edge bootstrap current continuously increases until the ELM crashes, while it saturates during the ELM cycle at high gas rates. The effect of current diffusion on the build-up of the edge current inter-ELM is assessed by simulating the Ohmic current contribution with the JETTO transport code. The simulations indicate that current diffusion contributes little to the time evolution of the total edge current in the second half of the ELM cycle and the total current is dominated by the bootstrap current. Therefore, current diffusion does not explain why JET-ILW type I ELMy pedestals at a high gas rate and high βN are found to be stable to peeling-ballooning modes.

    Original languageEnglish
    Article number085003
    JournalPlasma Physics and Controlled Fusion
    Volume60
    Issue number8
    DOIs
    Publication statusPublished - 13 Jun 2018
    MoE publication typeA1 Journal article-refereed

    Funding

    This work was supported by the Engineering and Physical Sciences Research Council (EP/ L01663X/1). This work has been carried out within the framework of the EUROfusion Consortium and has received funding from the Euratom research and training programme 2014–2018 under grant agreement No 633053.

    UN SDGs

    This output contributes to the following UN Sustainable Development Goals (SDGs)

    1. SDG 7 - Affordable and Clean Energy
      SDG 7 Affordable and Clean Energy

    Keywords

    • bootstrap current
    • current diffusion
    • edge current
    • ELMs
    • H-mode
    • JET-ILW
    • pedestal

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