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Last modified
11/23/2009 1:09:07 PM
Creation date
10/4/2006 10:26:53 PM
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Template:
Floodplain Documents
County
Pitkin
Community
Aspen
Title
Drainage Facility Capacity Analysis of City of Aspen
Date
9/1/1998
Prepared For
Aspen
Prepared By
WRC Engineering, Inc.
Floodplain - Doc Type
Project
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<br />relatively steep (i,e, alluvial fans), In this study the diffusive wave equations were <br />used by FLO-2D: <br />dh <br />~=~-- ~ <br />dx <br /> <br />and <br /> <br />dh <br />StY = Soy-- <br />dy <br /> <br />(5) <br /> <br />Flow depth, velocities, and discharges between adjacent nodes are calculated every <br />time step. The model makes a single sweep of the grid system, explicitly solving for <br />flow depth one node at a time for each time step, and storage volumes at each node <br />for both water and sediment are .computed. The inflow, outflow, and change in <br />storage across the entire grid system are assessed at the end of each time step to <br />ensure that volume is conserved within tolerance levels, If the volume is not <br />conserved sufficiently, the model will automatically reduce the time step and resolve <br />for flow depth at each node, <br /> <br />The rheological behavior of hyperconcentrated sediment flows involves the <br />interaction of several complex physical processes, including turbulence, fluid- <br />particle interaction, particle-particle interaction, and fluid viscosity, The total shear <br />stress in hyperconcentrated sediment flows, including mud floods and mudflows, can <br />be calculated from the summation of five shear stress components: <br /> <br />'='e+'me+'v+"M;d (6) <br />Where: , = Total Shear Stress <br /> 'e = Cohesive yield stress <br /> 'me = Mohr - Columb Shear Stress <br /> 'v = Viscous shear stress <br /> " = Turbulent shear stress <br /> 'd = Dispersive shear stress <br /> <br />! .. <br /> <br />The following quadratic equation was developed by the authors ofFLO- 2D and used <br />in FLO-2D to account for the various shear stresses. <br /> <br />( )' <br />dV dv <br />'t='ty+ll-+C - <br />dy dy <br /> <br />'t'y <br />TJ <br />dV <br />dy <br />C <br /> <br />(7) <br /> <br />Where: <br /> <br />= <br /> <br />~fnii~"viscosity <br />Rate of Shear <br /> <br />= <br /> <br />Inertial Shear Stress Coefficient <br /> <br />The first two tenus in Equation 7 are referred to as the Bingham shear stresses and <br /> <br />12 <br /> <br />, .- <br />
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