Laserfiche WebLink
<br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br /> <br />55 <br /> <br />begins when the material at the base of the bank starts to move, and this <br />occurs at a dimensionless shear stress of 0.06 (Parker, 1979). <br />The method used for this analysis is similar to that described previously <br />for the evaluation of coarse sediment transport, but the water surface slope <br />was used instead of the friction slope. The assumption that the water surface <br />slope is a reasonable estimate of the friction slope was tested at the flow <br />modeling sites, and results showed that they were similar. <br />Results <br />Cross-sections in the Grand Valley are generally wider and shallower <br />than in Ruby-Horsethief Canyon (Figs. 24 and 25, Tables 12 and 13). This is <br />reasonable since the Canyon reach is confined by bedrock walls in most areas <br />which results in a narrower and deeper channel. The bankfull dimensionless <br />shear stress ranges between 0.039 and 0.106 for the Grand Valley and between <br />0.0370 and 0.094 for Ruby-Horsethief Canyon. This range shows that there are <br />areas of relatively high and low shear stress at bankfull discharge which <br />would cause local scour and fill. This is expected since at high flows pools are <br />generally scoured and riffles accumulate coarse particles (Leopold et al., 1964). <br />The mean value for both reaches is near 0.06 which indicates that bankfull <br />flow causes significant transport of bed material, and that it produces a shear <br />stress near the threshold for bank erosion. More importantly, these values are <br />similar to bankfull results at the flow modeling sites where the dimensionless <br />shear stress is also near 0.06. This indicates that prescribed flows based upon <br />the flow modeling sites will yield similar results throughout the entire reach. <br />