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<br />Draft Final Completion Report to UDWR for Contract #93-1070. Amendment 3 <br /> <br /> <br />reach (Andrews and Nelson. 1989). Consequently, the roughness due to bars. bedforms, and saltating grains was <br /> <br />distributed throughout the channel rather than being restricted to the location where the roughness element extracts <br /> <br />momentum from the flow. <br /> <br />The Engelund- Hansen (1967) sediment transport equation was used for these Green River simulations. The <br />Engelund-Hansen relationship was developed for dunes in sand-bedded rivers. but was shown to be valid over the range <br />of flows including dunes. transition. standing waves, anti-dunes, and chute-and-pool flows (Engelund and Hansen, <br />1967). During this study. only ripples and dunes were observed in the sedimentary structures of the bank-attached bar <br />and on the fathometer traces, and these structures were composed of medium-sized sand (Appendix A). Unlike Yalin's <br />(1963) transport equation, the Engelund-Hansen equation for suspended load did not require additional bedform <br />information such as amplitude and wavelength. This approach was necessary for the Green River where a variety of <br /> <br />bedforms, from ripples to dunes superposed on bar forms, were present across the channel. The shear stress values, <br /> <br />calculated at all points of the matrix, were then used in the sediment transport equation to determine areas of erosion and <br />deposition. It was assumed that the modeled reach is in sedimentary equilibrium, that is, exactly as much sediment was <br />transported out of the reach as was transported into the reach. <br />While the Andrews and Nelson (1989) model was a physically-based 3-dimensional numerical model there <br />were several conditions for which this model did not function well (Nelson. 1994, pers. comm.). These conditions <br />include: <br /> <br />31 <br /> <br />1) when any part of the bar was emergent and where split flow around an island existed, and <br />2) low-flow conditions where areas of recirculation or stagnation existed. <br />Nelson (1994, pers. comm.) also noted that calibration of the model is necessary for each river reach to which it is <br />applied. <br />As a consequence of the first condition. only flows greater than the elevation of the highest elevation bar were <br />modeled. The second condition prevented the prediction of the locations of backwater habitat at low discharge. Thus, <br />the model was run only to predict the rate and style of bar building. <br /> <br />Model Modifications <br /> <br />Nelson (1994, pers. comm.) made modifications to the model to allow its use for the cross sections and <br /> <br /> <br />topography surveyed in 1993. Changes to the boundary conditions were necessary because the original version of the <br />