Fersiynau electronig

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  • Manuscript_Revised_black

    Llawysgrif awdur wedi’i dderbyn, 1.89 MB, dogfen-PDF

    Embargo yn dod i ben: 20/11/25

    Trwydded: CC BY-NC-ND Dangos trwydded

  • Bibliography_revised

    Llawysgrif awdur wedi’i dderbyn, 127 KB, dogfen-PDF

    Embargo yn dod i ben: 20/11/25

    Trwydded: CC BY-NC-ND Dangos trwydded

Dangosydd eitem ddigidol (DOI)

  • N Seiler
    CEA, DES, IRESNE, DTN, France
  • M Johnson
    Scalian, R&D Lab, France
  • L Vyskocil
    ÚJV Řež, Czech Republic
  • Y Vorobyov
    SSTC NRS, Ukraine
  • Walter Villanueva
  • M Abu Bakar
    PAEC, Pakistan
  • O Zhabin
    SSTC NRS, Ukraine
  • M Kratochvil
    ÚJV Řež, Czech Republic
  • B Bian
    KTH, Sweden
  • A Drouillet
    Scalian, R&D Lab, France
Convection within shallow pools of liquid metals heated from below is of significant interest for the In-Vessel Retention (IVR) strategy for Pressurised Water Reactors (PWR) as focusing of the lateral heat flux at the reactor wall presents a risk to the thermomechanical integrity of the reactor vessel. Under an IAEA Coordinated Research Project on corium melt retention, various international research institutions have performed CFD simulations to predict the thermal–hydraulic behaviour of a prototypic light metal layer of low Prandtl number (
) and high external Rayleigh number (
) dissipating heat from the free surface and at the lateral reactor wall. Various computational approaches including LES-WALE, LES-Smagorinsky and spectral-DNS were validated under the conditions of two BALI-Metal experiments in water (
), revealing promising agreement in the predicted repartition of the heat flux at the vertical and lateral boundaries. Simulations in a prototypic light metal layer indicated 30–34 % of heat dissipation due to thermal radiation at the free surface. Average thermal losses at the lateral wall corresponded to a focusing effect of 3.3–3.7 times the imposed heat flux. A spike in lateral heat flux close to the free surface equated to a local focusing effect 6-times the imposed heat flux from below. The fluid dynamics, driven largely by thermal losses at the reactor wall, were characterised by downwards acceleration adjacent to the lateral wall and ejection of a cold jet parallel to the lower boundary, forming a large convection cell comparable in size to the radius of the reactor.
Iaith wreiddiolSaesneg
Rhif yr erthygl113703
CyfnodolynNuclear Engineering and Design
Cyfrol431
Dyddiad ar-lein cynnar20 Tach 2024
Dynodwyr Gwrthrych Digidol (DOIs)
StatwsCyhoeddwyd - 1 Ion 2025
Gweld graff cysylltiadau