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Last modified
7/14/2009 5:02:34 PM
Creation date
5/20/2009 3:39:59 PM
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UCREFRP
UCREFRP Catalog Number
8251
Author
Rakowski, C. L. and J. C. Schmidt.
Title
The Geomorphic Basis of Colorado Squawfish Nursery Habitat in the Green River Near Ouray, Utah.
USFW Year
1996.
USFW - Doc Type
#93-1070,
Copyright Material
NO
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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 />
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