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Radiated energy fraction of SPI-induced disruptions at ASDEX Upgrade

The result's identifiers

  • Result code in IS VaVaI

    <a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F61389021%3A_____%2F25%3A00648043" target="_blank" >RIV/61389021:_____/25:00648043 - isvavai.cz</a>

  • Result on the web

    <a href="https://iopscience.iop.org/article/10.1088/1741-4326/adcbc0" target="_blank" >https://iopscience.iop.org/article/10.1088/1741-4326/adcbc0</a>

  • DOI - Digital Object Identifier

    <a href="http://dx.doi.org/10.1088/1741-4326/adcbc0" target="_blank" >10.1088/1741-4326/adcbc0</a>

Alternative languages

  • Result language

    angličtina

  • Original language name

    Radiated energy fraction of SPI-induced disruptions at ASDEX Upgrade

  • Original language description

    Future large tokamaks will operate at high plasma currents and high stored plasma energies. To ensure machine protection in case of a sudden loss of plasma confinement (major disruption), a large fraction of the magnetic and thermal energy must be radiated to reduce thermal loads. The disruption mitigation system for ITER is based on massive material injection in the form of shattered pellet injection (SPI). To support ITER, a versatile SPI system was installed at the tokamak ASDEX Upgrade (AUG). The AUG SPI features three independent pellet generation cells and guide tubes, and each was equipped with different shatter heads for the 2022 experimental campaign. We dedicated over 200 plasma discharges to the study of SPI plasma termination, and in this manuscript report on the results of bolometry (total radiation) analysis. We found, that the amount of neon inside the pellets is the dominant factor determining the radiated energy fraction ( f rad ). Large and fast fragments, produced by the 12.5 ∘ rectangular shatter head, lead to somewhat higher values of f rad compared to the 25° circular or rectangular heads. This effect is strongest for neon content of ≲ 3 × 10 20 neon atoms ( f neon ≲ 1.25 % neon) injected, where a lower normal velocity component (larger fragments) seems slightly beneficial. While full-sized, 8 mm diameter, 100% deuterium ( D 2 ) pellets lead to a disruption, the 4 mm or shortened 8 mm pellets of 100% D 2 did not. The disruption threshold for 100% D 2 is found to be around 1 × 10 22 deuterium molecules inside the pellet. While the radiated energy fraction of non-disruptive SPI is below 20%, this is increased to 40% during the thermal quench and vertical displacement event phase of the disruptive injections. For deuterium-neon-mix pellets, f radvalues of ⩽ 90 % are observed, and the curve saturates around 80% already for 10% neon mixed into the 8 mm pellets ( 2 × 10 21 neon atoms).

  • 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

    I - Institucionalni podpora na dlouhodoby koncepcni rozvoj vyzkumne organizace

Others

  • Publication year

    2025

  • Confidentiality

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

Data specific for result type

  • Name of the periodical

    Nuclear Fusion

  • ISSN

    0029-5515

  • e-ISSN

    1741-4326

  • Volume of the periodical

    65

  • Issue of the periodical within the volume

    5

  • Country of publishing house

    US - UNITED STATES

  • Number of pages

    15

  • Pages from-to

    056036

  • UT code for WoS article

    001476013700001

  • EID of the result in the Scopus database

    2-s2.0-105003695502