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    Cohesionless Fine‐Sediment Bed Forms in Shallow Flows

    Source: Journal of Hydraulic Engineering:;1992:;Volume ( 118 ):;issue: 005
    Author:
    Peter A. Mantz
    DOI: 10.1061/(ASCE)0733-9429(1992)118:5(743)
    Publisher: American Society of Civil Engineers
    Abstract: Bed‐form data from laboratory experiments using cohesionless, fine silica solids in shallow water flows are analyzed to find dimenionless relationships for geometry and friction factor. With increasing flow discharge over a stationary flat bed, the bed‐form sequence is primary ripples, barchanoid and linguoid ripples (secondary ripples), ripples on dunes (for silt grades only), and a moving flat bed. The primaries develop from the incipient transport stress, otherwise called the primary threshold. By extrapolating dimensionless bedform length and height data to this threshold, it is shown that the geometry is proportional to the depth of the viscous sublayer thickness. The secondaries develop from a secondary threshold, which is an approximate constant stress condition at which incipient suspension also begins. The ripples on dune form is associated with a tertiary threshold for which the dimensionless stress ratio
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      Cohesionless Fine‐Sediment Bed Forms in Shallow Flows

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    contributor authorPeter A. Mantz
    date accessioned2017-05-08T20:41:29Z
    date available2017-05-08T20:41:29Z
    date copyrightMay 1992
    date issued1992
    identifier other%28asce%290733-9429%281992%29118%3A5%28743%29.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/23649
    description abstractBed‐form data from laboratory experiments using cohesionless, fine silica solids in shallow water flows are analyzed to find dimenionless relationships for geometry and friction factor. With increasing flow discharge over a stationary flat bed, the bed‐form sequence is primary ripples, barchanoid and linguoid ripples (secondary ripples), ripples on dunes (for silt grades only), and a moving flat bed. The primaries develop from the incipient transport stress, otherwise called the primary threshold. By extrapolating dimensionless bedform length and height data to this threshold, it is shown that the geometry is proportional to the depth of the viscous sublayer thickness. The secondaries develop from a secondary threshold, which is an approximate constant stress condition at which incipient suspension also begins. The ripples on dune form is associated with a tertiary threshold for which the dimensionless stress ratio
    publisherAmerican Society of Civil Engineers
    titleCohesionless Fine‐Sediment Bed Forms in Shallow Flows
    typeJournal Paper
    journal volume118
    journal issue5
    journal titleJournal of Hydraulic Engineering
    identifier doi10.1061/(ASCE)0733-9429(1992)118:5(743)
    treeJournal of Hydraulic Engineering:;1992:;Volume ( 118 ):;issue: 005
    contenttypeFulltext
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