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    Freezing of a Salt Solution in a Packed Bed

    Source: Journal of Offshore Mechanics and Arctic Engineering:;1996:;volume( 118 ):;issue: 001::page 79
    Author:
    S. Chellaiah
    ,
    H. Singh
    DOI: 10.1115/1.2828805
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: There are many natural processes and technological applications that involve the solidification of a binary solution saturating a porous matrix. Some of them are: natural freezing and artificial freezing (for construction purposes) of soil, oil exploration in cold regions, and processing and preservation of food. This paper presents the results of a fundamental study of freezing of a binary salt solution saturating a packed bed. An aqueous sodium chloride solution (of noneutectic composition) constituted the binary solution and spherical glass beads constituted the packed bed. The freezing was initiated at one of the vertical walls of a rectangular cavity. The temperature distributions in the solid, mush, and liquid regions were recorded using thermocouples. The concentration of salt was determined using a sample withdrawal technique in conjunction with a refractometer and a calibration chart. There was buoyancy-driven convective flow generated and sustained by the thermal and solutal gradients. The effect of this flow on the freezing process was significant. The morphology of the freezing fronts, the temperature and salt concentration profiles, and the rate of freezing were all influenced by the flow. Even in experiments with an initial superheat of 10°C, it was found that the effect of flow was considerable. For even though the fluid flows through the interstitial spaces in the porous matrix, the permeability was large for balls of 0.5-in. diameter. With a superheat of 20°C, the convection was vigorous and the rate of freezing was retarded considerably. The salt rejected during freezing was redistributed by the flow. At later times, a stable solute-rich region formed at the bottom of test cell where the concentration decreased with height. The amount of salt rejected was directly influenced by the rate of freezing, which in turn was controlled by the superheat and the permeability of packed bed.
    keyword(s): Freezing , Flow (Dynamics) , Permeability , Preservation , Construction , Glass beads , Space , Cold climates , Convection , Solidification , Calibration , Cavities , Food products , Gradients , Sodium , Soil , Temperature distribution , Thermocouples , Buoyancy , Temperature AND Fluid dynamics ,
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      Freezing of a Salt Solution in a Packed Bed

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    http://yetl.yabesh.ir/yetl1/handle/yetl/117509
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    • Journal of Offshore Mechanics and Arctic Engineering

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    contributor authorS. Chellaiah
    contributor authorH. Singh
    date accessioned2017-05-08T23:51:19Z
    date available2017-05-08T23:51:19Z
    date copyrightFebruary, 1996
    date issued1996
    identifier issn0892-7219
    identifier otherJMOEEX-28106#79_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/117509
    description abstractThere are many natural processes and technological applications that involve the solidification of a binary solution saturating a porous matrix. Some of them are: natural freezing and artificial freezing (for construction purposes) of soil, oil exploration in cold regions, and processing and preservation of food. This paper presents the results of a fundamental study of freezing of a binary salt solution saturating a packed bed. An aqueous sodium chloride solution (of noneutectic composition) constituted the binary solution and spherical glass beads constituted the packed bed. The freezing was initiated at one of the vertical walls of a rectangular cavity. The temperature distributions in the solid, mush, and liquid regions were recorded using thermocouples. The concentration of salt was determined using a sample withdrawal technique in conjunction with a refractometer and a calibration chart. There was buoyancy-driven convective flow generated and sustained by the thermal and solutal gradients. The effect of this flow on the freezing process was significant. The morphology of the freezing fronts, the temperature and salt concentration profiles, and the rate of freezing were all influenced by the flow. Even in experiments with an initial superheat of 10°C, it was found that the effect of flow was considerable. For even though the fluid flows through the interstitial spaces in the porous matrix, the permeability was large for balls of 0.5-in. diameter. With a superheat of 20°C, the convection was vigorous and the rate of freezing was retarded considerably. The salt rejected during freezing was redistributed by the flow. At later times, a stable solute-rich region formed at the bottom of test cell where the concentration decreased with height. The amount of salt rejected was directly influenced by the rate of freezing, which in turn was controlled by the superheat and the permeability of packed bed.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleFreezing of a Salt Solution in a Packed Bed
    typeJournal Paper
    journal volume118
    journal issue1
    journal titleJournal of Offshore Mechanics and Arctic Engineering
    identifier doi10.1115/1.2828805
    journal fristpage79
    journal lastpage85
    identifier eissn1528-896X
    keywordsFreezing
    keywordsFlow (Dynamics)
    keywordsPermeability
    keywordsPreservation
    keywordsConstruction
    keywordsGlass beads
    keywordsSpace
    keywordsCold climates
    keywordsConvection
    keywordsSolidification
    keywordsCalibration
    keywordsCavities
    keywordsFood products
    keywordsGradients
    keywordsSodium
    keywordsSoil
    keywordsTemperature distribution
    keywordsThermocouples
    keywordsBuoyancy
    keywordsTemperature AND Fluid dynamics
    treeJournal of Offshore Mechanics and Arctic Engineering:;1996:;volume( 118 ):;issue: 001
    contenttypeFulltext
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