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    Singular Perturbation Theory for Melting or Freezing in Finite Domains Initially Not at the Fusion Temperature

    Source: Journal of Applied Mechanics:;1977:;volume( 044 ):;issue: 001::page 25
    Author:
    S. Weinbaum
    ,
    L. M. Jiji
    DOI: 10.1115/1.3424008
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: This paper treats the problem of the inward solidification at large Stefan number 1/ε, ε = CP (Ti − Tf )/L , of a finite slab which is initially at an arbitrary temperature Ti above the melting point. The face at which the heat is removed is maintained at a constant temperature below fusion while the opposite face is either (a) insulated or (b) kept at the initial temperature. Perturbation series solutions in ε are obtained for both the short-time scale characterizing the transient diffusion in the liquid phase and the long-time scale characterizing the interface motion. The asymptotic matching of the two series solutions shows that to O(ε1/2 ) the short-time series solution for interface motion for the insulated Case (a) is uniformly valid for all time. A singular perturbation theory is, however, required for the isothermal Case (b) since the interface motion is affected to this order by the inhomogeneous temperature distribution in the liquid phase.
    keyword(s): Temperature , Freezing , Melting , Perturbation theory , Motion , Slabs , Diffusion (Physics) , Temperature distribution , Solidification , Melting point AND Heat ,
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      Singular Perturbation Theory for Melting or Freezing in Finite Domains Initially Not at the Fusion Temperature

    URI
    http://yetl.yabesh.ir/yetl1/handle/yetl/89586
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    contributor authorS. Weinbaum
    contributor authorL. M. Jiji
    date accessioned2017-05-08T23:02:24Z
    date available2017-05-08T23:02:24Z
    date copyrightMarch, 1977
    date issued1977
    identifier issn0021-8936
    identifier otherJAMCAV-26068#25_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/89586
    description abstractThis paper treats the problem of the inward solidification at large Stefan number 1/ε, ε = CP (Ti − Tf )/L , of a finite slab which is initially at an arbitrary temperature Ti above the melting point. The face at which the heat is removed is maintained at a constant temperature below fusion while the opposite face is either (a) insulated or (b) kept at the initial temperature. Perturbation series solutions in ε are obtained for both the short-time scale characterizing the transient diffusion in the liquid phase and the long-time scale characterizing the interface motion. The asymptotic matching of the two series solutions shows that to O(ε1/2 ) the short-time series solution for interface motion for the insulated Case (a) is uniformly valid for all time. A singular perturbation theory is, however, required for the isothermal Case (b) since the interface motion is affected to this order by the inhomogeneous temperature distribution in the liquid phase.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleSingular Perturbation Theory for Melting or Freezing in Finite Domains Initially Not at the Fusion Temperature
    typeJournal Paper
    journal volume44
    journal issue1
    journal titleJournal of Applied Mechanics
    identifier doi10.1115/1.3424008
    journal fristpage25
    journal lastpage30
    identifier eissn1528-9036
    keywordsTemperature
    keywordsFreezing
    keywordsMelting
    keywordsPerturbation theory
    keywordsMotion
    keywordsSlabs
    keywordsDiffusion (Physics)
    keywordsTemperature distribution
    keywordsSolidification
    keywordsMelting point AND Heat
    treeJournal of Applied Mechanics:;1977:;volume( 044 ):;issue: 001
    contenttypeFulltext
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