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    Therporaoustic Convection: Modeling and Analysis of Flow, Thermal, and Energy Fields

    Source: Journal of Heat Transfer:;2009:;volume( 131 ):;issue: 010::page 101011
    Author:
    Shohel Mahmud
    ,
    Roydon Andrew Fraser
    DOI: 10.1115/1.3180705
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: The problem of therporacoustic (thermal-porous-acoustic) convection near a porous medium, representative of a stack in a thermoacoustic engine/refrigerator, is modeled and analyzed in this paper. Assumptions (e.g., long wave, short stack, and small amplitude oscillation) are made to enable simplification of the governing unsteady-compressible-viscous forms of the continuity, momentum, and energy equations to achieve analytical solutions for the fluctuating velocity and temperature and the complex Nusselt number. Boundary walls are assumed to be very thin in thickness and the conduction heat transfer inside the boundary walls are neglected in this paper. The derived analytical results are expressed mainly in terms of the Darcy number (Da), critical temperature gradient ratio (Γ0), Swift number (Sw), Prandtl number (Pr), and modified Rott’s and Swift’s parameters (fν and fk). The real part of the fluctuating flow complex Nusselt number approaches to the steady result, as reported in the literature, at the zero frequency limit. While in the high frequency limit, the real part of the complex Nusselt number matches well with the limit obtained by other oscillating flow researchers with slight differences explained by additional terms included in this work. A wave equation for the pressure fluctuation is modeled by combining the continuity, momentum, and energy equations and subsequent integrations which, in the inviscid no-stack limit, approaches the Helmholtz wave equation. Based on the derived energy flux density equation performance plots are proposed, which give the Swift number at the maximum energy transfer (Sw0) for a given Γ0 and Da.
    keyword(s): Flow (Dynamics) , Temperature , Heat transfer , Fluids , Channels (Hydraulic engineering) , Porous materials , Density , Convection , Equations , Temperature gradients , Pressure , Thermoacoustic devices , Wave equations AND Modeling ,
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      Therporaoustic Convection: Modeling and Analysis of Flow, Thermal, and Energy Fields

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    http://yetl.yabesh.ir/yetl1/handle/yetl/140964
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    contributor authorShohel Mahmud
    contributor authorRoydon Andrew Fraser
    date accessioned2017-05-09T00:33:36Z
    date available2017-05-09T00:33:36Z
    date copyrightOctober, 2009
    date issued2009
    identifier issn0022-1481
    identifier otherJHTRAO-27872#101011_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/140964
    description abstractThe problem of therporacoustic (thermal-porous-acoustic) convection near a porous medium, representative of a stack in a thermoacoustic engine/refrigerator, is modeled and analyzed in this paper. Assumptions (e.g., long wave, short stack, and small amplitude oscillation) are made to enable simplification of the governing unsteady-compressible-viscous forms of the continuity, momentum, and energy equations to achieve analytical solutions for the fluctuating velocity and temperature and the complex Nusselt number. Boundary walls are assumed to be very thin in thickness and the conduction heat transfer inside the boundary walls are neglected in this paper. The derived analytical results are expressed mainly in terms of the Darcy number (Da), critical temperature gradient ratio (Γ0), Swift number (Sw), Prandtl number (Pr), and modified Rott’s and Swift’s parameters (fν and fk). The real part of the fluctuating flow complex Nusselt number approaches to the steady result, as reported in the literature, at the zero frequency limit. While in the high frequency limit, the real part of the complex Nusselt number matches well with the limit obtained by other oscillating flow researchers with slight differences explained by additional terms included in this work. A wave equation for the pressure fluctuation is modeled by combining the continuity, momentum, and energy equations and subsequent integrations which, in the inviscid no-stack limit, approaches the Helmholtz wave equation. Based on the derived energy flux density equation performance plots are proposed, which give the Swift number at the maximum energy transfer (Sw0) for a given Γ0 and Da.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleTherporaoustic Convection: Modeling and Analysis of Flow, Thermal, and Energy Fields
    typeJournal Paper
    journal volume131
    journal issue10
    journal titleJournal of Heat Transfer
    identifier doi10.1115/1.3180705
    journal fristpage101011
    identifier eissn1528-8943
    keywordsFlow (Dynamics)
    keywordsTemperature
    keywordsHeat transfer
    keywordsFluids
    keywordsChannels (Hydraulic engineering)
    keywordsPorous materials
    keywordsDensity
    keywordsConvection
    keywordsEquations
    keywordsTemperature gradients
    keywordsPressure
    keywordsThermoacoustic devices
    keywordsWave equations AND Modeling
    treeJournal of Heat Transfer:;2009:;volume( 131 ):;issue: 010
    contenttypeFulltext
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