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

The result's identifiers

  • Result code in IS VaVaI

    <a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F00216208%3A11320%2F20%3A10439903" target="_blank" >RIV/00216208:11320/20:10439903 - isvavai.cz</a>

  • Alternative codes found

    RIV/61389021:_____/20:00538142 RIV/68407700:21340/20:00347601

  • Result on the web

    <a href="https://verso.is.cuni.cz/pub/verso.fpl?fname=obd_publikace_handle&handle=9CCzzSjBvM" target="_blank" >https://verso.is.cuni.cz/pub/verso.fpl?fname=obd_publikace_handle&handle=9CCzzSjBvM</a>

  • DOI - Digital Object Identifier

    <a href="http://dx.doi.org/10.1063/5.0021154" target="_blank" >10.1063/5.0021154</a>

Alternative languages

  • Result language

    angličtina

  • Original language name

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

  • Original language description

    The 3-D field induced relativistic runaway electron (RE) loss has been simulated for DIII-D and COMPASS 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 1kG level of magnetic field perturbation produced by a fast growing n=1 resistive kink instability. This complete 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 (&gt;10%) RE loss in COMPASS post-disruption plasmas, consistent with experimental observations in the 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 vs the machine size and the toroidal magnetic field. In the modeling, the lost REs due to 3-D fields deposit onto the limiting surfaces of the devices. Distributions of the lost REs to the limiting surface show a poloidally peaked profile near the high-field-side in both DIII-D and COMPASS, covering about 100 degrees poloidal angle. A 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.

  • Czech name

  • Czech description

Classification

  • Type

    J<sub>imp</sub> - Article in a specialist periodical, which is included in the Web of Science database

  • CEP classification

  • OECD FORD branch

    10305 - Fluids and plasma physics (including surface physics)

Result continuities

  • Project

  • Continuities

    S - Specificky vyzkum na vysokych skolach

Others

  • Publication year

    2020

  • Confidentiality

    S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů

Data specific for result type

  • Name of the periodical

    Physics of Plasmas

  • ISSN

    1070-664X

  • e-ISSN

  • Volume of the periodical

    27

  • Issue of the periodical within the volume

    10

  • Country of publishing house

    US - UNITED STATES

  • Number of pages

    18

  • Pages from-to

    102507

  • UT code for WoS article

    000582511200003

  • EID of the result in the Scopus database

    2-s2.0-85092727738