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    The effect of the rear cavity wall ingot shape on the evolution of the liquid–solid interface during melting for the eutectic Pt-C

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    TheEffectoftheRearCa ... (641.2Kb)
    Identificadores
    URI: http://hdl.handle.net/10902/9740
    DOI: 10.1007/s10765-013-1555-3
    ISSN: 0195-928X
    ISSN: 1572-9567
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    Autoría
    Castro Alonso, Pablo BernardoAutoridad Unican; Bloembergen, Pieter; Arroyo Gutiérrez, AlbertoAutoridad Unican
    Fecha
    2014-04
    Derechos
    © Springer. The final publication is available at Springer via https://doi.org/10.1007/s10765-013-1555-3
    Publicado en
    International Journal of Thermophysics, 2014, 35(3), 438–445
    Editorial
    Springer
    Enlace a la publicación
    https://doi.org/10.1007/s10765-013-1555-3
    Palabras clave
    High temperature fixed points
    Liquid-solid interface
    Shape effect
    Resumen/Abstract
    When characterizing high-temperature fixed points, the fraction of the melting time of the regular part of the plateau with respect to the total melting time, is critical. Maximizing the melting duration minimizes the uncertainty associated with the determination of the fixed-point temperature. One factor that affects this quality is the effect of the thermal bridging between the external and internal surfaces of the ingot enclosed by the cell. This paper presents the results of simulations for the eutectic Pt-C, investigating the effects of different ingot shapes on the duration of the melt plateau. It was found that the formation of a thermal bridge from the rear of the blackbody cavity toward the outer surface of the ingot was critical and that its formation could be delayed or suppressed through a proper choice of the ingot shape. The shapes considered included, firstly, the shape of the rear of the cavity, in contact with the ingot, either cone-shaped or dome-shaped, and secondly, the inside rear surface of the cell, in contact with the ingot, being a cone, a convex dome, or flat. The presence of impurities in the alloy was taken into consideration, and its influence in the evolution of the liquid–solid interface compared with that for the pure alloy. The effect of changing the thermal isolation of the cell, at its front side, was also considered. A dome-shaped surface for the rear of the cavity was found to be more favorable for the development of a regular melting front, in conjunction with the segregation of impurities during melting. At the rear of the cell, a flat surface ensures the back wall is the last to experience thermal bridging, resulting in more extended melting plateaus.
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    UNIVERSIDAD DE CANTABRIA

    Repositorio realizado por la Biblioteca Universitaria utilizando DSpace software
    Contacto | Sugerencias
    Metadatos sujetos a:licencia de Creative Commons Reconocimiento 4.0 España