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    Steady State Heat Conduction in Exchanger Tubes by Using the Meshfree Boundary Integral Equation Method: Conduction Shape Factor and Degenerate Scale

    Source: ASME Journal of Heat and Mass Transfer:;2023:;volume( 145 ):;issue: 011::page 111901-1
    Author:
    Lee, Jia-Wei
    ,
    Yang, Hung-Wen
    ,
    Chen, Jeng-Tzong
    DOI: 10.1115/1.4062760
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: Regarding the steady-state heat conduction problem in exchanger tubes, the meshfree boundary integral equation method is employed to determine the conduction shape factor in this paper. Different from the conventional boundary element method, the present method is free of mesh generation. After using the parametric function to represent the boundary contour and adopting the Gaussian quadrature, only collocating points on the boundary is required to obtain the linear algebraic equations. By introducing the local exact solution, the singular integral in the sense of the Cauchy principal value can be novelly determined. In addition, the boundary layer effect due to the nearly singular integral in the boundary integral equation can be dealt with. Two cases of different boundary conditions are considered. One is the isothermal condition on both the inner and outer surfaces. The other is the isothermal condition on the inner surface and the convection condition on the outer surface. Besides, numerical instability is found and the nonuniqueness solution due to the degenerate scale is examined by calculating the conduction shape factor and the temperature on the outer surface.
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      Steady State Heat Conduction in Exchanger Tubes by Using the Meshfree Boundary Integral Equation Method: Conduction Shape Factor and Degenerate Scale

    URI
    http://yetl.yabesh.ir/yetl1/handle/yetl/4294396
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    contributor authorLee, Jia-Wei
    contributor authorYang, Hung-Wen
    contributor authorChen, Jeng-Tzong
    date accessioned2023-11-29T18:49:05Z
    date available2023-11-29T18:49:05Z
    date copyright7/17/2023 12:00:00 AM
    date issued7/17/2023 12:00:00 AM
    date issued2023-07-17
    identifier issn2832-8450
    identifier otherht_145_11_111901.pdf
    identifier urihttp://yetl.yabesh.ir/yetl1/handle/yetl/4294396
    description abstractRegarding the steady-state heat conduction problem in exchanger tubes, the meshfree boundary integral equation method is employed to determine the conduction shape factor in this paper. Different from the conventional boundary element method, the present method is free of mesh generation. After using the parametric function to represent the boundary contour and adopting the Gaussian quadrature, only collocating points on the boundary is required to obtain the linear algebraic equations. By introducing the local exact solution, the singular integral in the sense of the Cauchy principal value can be novelly determined. In addition, the boundary layer effect due to the nearly singular integral in the boundary integral equation can be dealt with. Two cases of different boundary conditions are considered. One is the isothermal condition on both the inner and outer surfaces. The other is the isothermal condition on the inner surface and the convection condition on the outer surface. Besides, numerical instability is found and the nonuniqueness solution due to the degenerate scale is examined by calculating the conduction shape factor and the temperature on the outer surface.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleSteady State Heat Conduction in Exchanger Tubes by Using the Meshfree Boundary Integral Equation Method: Conduction Shape Factor and Degenerate Scale
    typeJournal Paper
    journal volume145
    journal issue11
    journal titleASME Journal of Heat and Mass Transfer
    identifier doi10.1115/1.4062760
    journal fristpage111901-1
    journal lastpage111901-15
    page15
    treeASME Journal of Heat and Mass Transfer:;2023:;volume( 145 ):;issue: 011
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
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