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    New Temperature and Heat Loss Charts for One-Dimensional, Transient Heat Conduction

    Source: ASME Journal of Heat and Mass Transfer:;2022:;volume( 145 ):;issue: 001::page 14502-1
    Author:
    Wei, Tie
    ,
    Abraham, John
    ,
    Wang, Yanxing
    DOI: 10.1115/1.4055817
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: New temperature and heat loss charts have been created for one-dimensional, transient conduction. In the new charts, time is scaled by a weighted sum of the lumped capacitance time scale tLC and the diffusion time scale tdiff: tref=a tLC+b tdiff, where a and b are constants. As the Biot number approaches zero, the diffusion time scale is much smaller than the lumped capacitance time scale (tdiff≪tLC), so the new time scale is equivalent to the lumped capacitance time scale. As the Biot number approaches infinity, the diffusion time scale is much larger than the lumped capacitance time scale (tdiff≫tLC), so the new time scale is equivalent to the diffusion time scale. Using the new time scale, the dimensionless temperature excess and heat loss fraction can be compactly presented in a single plot. The new time scale and associated plots cast new light on some fundamental aspects of the study of conductive heat transfer, and simplify the design process.
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      New Temperature and Heat Loss Charts for One-Dimensional, Transient Heat Conduction

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    contributor authorWei, Tie
    contributor authorAbraham, John
    contributor authorWang, Yanxing
    date accessioned2023-11-29T18:43:54Z
    date available2023-11-29T18:43:54Z
    date copyright11/17/2022 12:00:00 AM
    date issued11/17/2022 12:00:00 AM
    date issued2022-11-17
    identifier issn2832-8450
    identifier otherht_145_01_014502.pdf
    identifier urihttp://yetl.yabesh.ir/yetl1/handle/yetl/4294348
    description abstractNew temperature and heat loss charts have been created for one-dimensional, transient conduction. In the new charts, time is scaled by a weighted sum of the lumped capacitance time scale tLC and the diffusion time scale tdiff: tref=a tLC+b tdiff, where a and b are constants. As the Biot number approaches zero, the diffusion time scale is much smaller than the lumped capacitance time scale (tdiff≪tLC), so the new time scale is equivalent to the lumped capacitance time scale. As the Biot number approaches infinity, the diffusion time scale is much larger than the lumped capacitance time scale (tdiff≫tLC), so the new time scale is equivalent to the diffusion time scale. Using the new time scale, the dimensionless temperature excess and heat loss fraction can be compactly presented in a single plot. The new time scale and associated plots cast new light on some fundamental aspects of the study of conductive heat transfer, and simplify the design process.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleNew Temperature and Heat Loss Charts for One-Dimensional, Transient Heat Conduction
    typeJournal Paper
    journal volume145
    journal issue1
    journal titleASME Journal of Heat and Mass Transfer
    identifier doi10.1115/1.4055817
    journal fristpage14502-1
    journal lastpage14502-6
    page6
    treeASME Journal of Heat and Mass Transfer:;2022:;volume( 145 ):;issue: 001
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
    نرم افزار کتابخانه دیجیتال "دی اسپیس" فارسی شده توسط یابش برای کتابخانه های ایرانی | تماس با یابش
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