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<br />was tested against hand computations for simpl'9' verification (See "Model Confirmation' <br />SElction). <br /> <br />The equilibrium sediment transport values lor each discharge were aggregated into an event <br />hydrograph and a total sediment volume for each eVElnt was determined. The individual event <br />sediment yield estimates were integrated to determine an average annual sediment yield for <br />comparison to the previously computed PSIA methodology e,stimate of average annual <br />sediment yield. This integration was performed by plotting a curve of total sediment yield for <br />each event against the probability of the event recurrence and determining the arEla beneath the <br />curve which represents average annual sediment yield. (See 'Ave I~nnual Yield' Sec;tion.) <br /> <br />fA,NjDIKE SYSTEM ANALYSIS <br /> <br />Th'3 previously described hydrograph and event specific sediment inflow was used to evaluate <br />the, effects of the West Range Wash Dike system 011 the sediment transport oj the 1oo-year <br />ElVElnt. HEC-6 requires that a hydrograph and a sediment rating curve bEl input into the model <br />as a boundary condition. The sediment yield r.ating curve was developed basEld on the fan <br />Elquilibrium transport capacity computations used to develop the event specific yield estimates <br />described above. <br /> <br />ThEl HEC-6 model began at the apex of the alluvial fan with the apex flow hydrogn~ph and an <br />assumed sediment load. (See "System MOdel" Section.) Flows down the alluvial fan were <br />modeled USing the previousiy described channel of constant cross-section. Flows were <br />modeled down the fan where they reached equilibrium and Wl3re eventually interc:epted by the <br />West Range Wash Dike. The model cross-section was modified to' reflect the geometry of the <br />channel along the upstream toe of the dike and the slope along the dike as it traverses the fan. <br /> <br />A 1:20 foot wide unlined channel with 3:1 side slopes was assumed along the upstream toe 01 <br />the dike. Two longitudinal bed Slopes were simulated which l"epresented the extremes of the <br />conditions encountered along the dike. (0.5 percent and 1.0 pelJ'cent). <br /> <br />HEC-6 determines the equilibrium sediment transport down the fan and, based on a <br />comparison with the computed equilibrium sediment transport along the dike, the total volume <br />of deposition is computed for each time step. Because 01 intermediate cCJmputational <br />instabilities, it was not possible to determine the total volume of deposition which occurred at <br />the peak flow by interpreting HEC-6 directly. An intermediate computation basecj on a mass <br />curve of sediment transport was required which determined that ~~8% of the total deposition <br />occurred at the peak discharge. (See "Deposition Percelntage" Section) <br /> <br />HEC-6 computes equilibrium transport at each cross-section and Ciannot distribute deposition <br />throlJgh a channel reach. The methodology prese,nted in Desi(ln of Small Dams for evaluating <br />the (leometry and longitudinal length of a scour hole was modified slightly and applied here to <br />estimate the length of deposition and the maximum depth of the, deposited materials at the 100- <br />yr pElak flow (See "Transition Model" section). This methodology was compared to a parabOlic <br />vertil~al curve of a comparable length and resulted in a good correlation for the maximum <br />depth. A transition length of approximately 1,100 feet Cind a depth 01' deposition of 5.9 feet was <br />computed. <br /> <br />WATER SURFACE PROFILE DETERMINATION <br /> <br />The computed transition and deposition were incorporated into a HEC-2 run to deltermine the <br />water surface through the transition section. A horizontal transition between the re,ctangular <br />