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    Numerical Modeling of Mudflows

    Source: Journal of Hydraulic Engineering:;1997:;Volume ( 123 ):;issue: 007
    Author:
    Dominique Laigle
    ,
    Philippe Coussot
    DOI: 10.1061/(ASCE)0733-9429(1997)123:7(617)
    Publisher: American Society of Civil Engineers
    Abstract: To predict mudflow dynamics a numerical model based on shallow-water equations is developed. Previous work has shown that mudflow behavior can be well represented by a Herschel-Bulkley model. In a laminar regime, generally observed in practice, a wall friction force expression has been theoretically deduced for steady uniform flows. For unsteady flows the wall friction force is assumed to be equal to the resistance of a steady uniform flow with the same depth and mean velocity. The numerical model parameters, directly deduced from Herschel-Bulkley model, are determined independently by rheological measurements. Because of the lack of precise field data, experimental results obtained on a physical model are used in order to validate the numerical model. The main features of the experimental transient flows carried out in a laboratory flume are, for some identified conditions, in fairly good agreement with numerical model predictions, without any additional parameter fitting.
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      Numerical Modeling of Mudflows

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    http://yetl.yabesh.ir/yetl1/handle/yetl/24469
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    contributor authorDominique Laigle
    contributor authorPhilippe Coussot
    date accessioned2017-05-08T20:42:52Z
    date available2017-05-08T20:42:52Z
    date copyrightJuly 1997
    date issued1997
    identifier other%28asce%290733-9429%281997%29123%3A7%28617%29.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/24469
    description abstractTo predict mudflow dynamics a numerical model based on shallow-water equations is developed. Previous work has shown that mudflow behavior can be well represented by a Herschel-Bulkley model. In a laminar regime, generally observed in practice, a wall friction force expression has been theoretically deduced for steady uniform flows. For unsteady flows the wall friction force is assumed to be equal to the resistance of a steady uniform flow with the same depth and mean velocity. The numerical model parameters, directly deduced from Herschel-Bulkley model, are determined independently by rheological measurements. Because of the lack of precise field data, experimental results obtained on a physical model are used in order to validate the numerical model. The main features of the experimental transient flows carried out in a laboratory flume are, for some identified conditions, in fairly good agreement with numerical model predictions, without any additional parameter fitting.
    publisherAmerican Society of Civil Engineers
    titleNumerical Modeling of Mudflows
    typeJournal Paper
    journal volume123
    journal issue7
    journal titleJournal of Hydraulic Engineering
    identifier doi10.1061/(ASCE)0733-9429(1997)123:7(617)
    treeJournal of Hydraulic Engineering:;1997:;Volume ( 123 ):;issue: 007
    contenttypeFulltext
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