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To examine the importance of spatial variations in grain size, the modeled estimates of r* <br />were re-calculated using a "local" grain size for each cross section. The local grain size was <br />determined by taking the average of several values, centered around the section. Calculations for <br />higher flows were based on samples from the thalweg as well as exposed bar surfaces, since <br />these areas would both be under water. Calculations for lower flows were based only on samples <br />from the thalweg. The effect of using spatially variable grain sizes in the model is to reduce the <br />estimates of r* slightly, as shown in Figure 27. The inclusion of coarser sediment in certain <br />areas of the channel has the most noticeable effect on flow conditions in the riffle, and then <br />mostly only in the intermediate range of flows, 125-224 m3/s. At those flows, the shear stress <br />through the riffle is quite high because the energy slope is high; however, when the shear stress <br />produced by those flows is balanced against the coarser bed grain sizes, the modeled values of r* <br />through the riffle decrease substantially (Fig. 27). The net effect of using spatially variable (and <br />generally coarser) grain sizes is to reduce the potential for bed load transport at flows much less <br />than about 300 m3/s, thus that value is retained as the threshold discharge for initial motion. <br /> <br /> 0.04 <br />N <br />0.03 <br /> <br /> <br />m <br />O <br />z <br />y 0.02 <br /> <br /> <br />C <br />O <br /> <br /> 0.01 <br />E <br />0 <br /> <br /> 0.00 <br /> 0 100 200 300 400 500 <br /> Discharge (m3/s) <br />Figure 27. Relation between dimensionless shear stress and discharge, RM 176, <br />after adjusting for spatial variations in grain size. <br /> i • <br /> ? _ QQ <br /> <br /> <br /> <br /> <br /> <br />? <br />.ao <br />y 0.0025xo <br />• R2 = 0.63 <br />54