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As the plots on the preceding page show, the flow depth through the study reach <br />increases rapidly over the range of low to intermediate discharges, and more slowly thereafter. It <br />is also evident that the water-surface profile becomes more uniform as the depth and discharge <br />increase. The adjustments in depth and slope both influence changes in boundary shear stress, T, <br />which are used as the basis for estimating thresholds for bed load transport. Recall that the <br />boundary shear stress is calculated using equation 3, with the observed depth, h, and the modeled <br />energy slope, Se. Figure 25 plots the modeled values of boundary shear stress versus discharge <br />for the range of observed flows. The individual points represent the modeled values of boundary <br />shear stress at each of the cross sections in the study reach, and the smooth curve represents the <br />best-fit relation. <br /> <br />45 <br /> <br />40 <br />35 <br />= • = s • <br />N <br /> <br />? 30 • <br /> <br />25 <br /> <br />U)20 • <br />cc 15 <br />v ? y _ 2.932 .ao <br />? 1 0 <br />5 • • R2 = 0.51 <br /> <br /> <br />0 <br /> <br />0 100 200 300 400 500 <br />Discharge (m3/s) <br />Figure 25. Relation between shear stress and discharge, RM 176 <br />The results shown above indicate that, for a given discharge, the shear stress can vary <br />appreciably from one cross section to another. The greatest range in shear stress occurs at a <br />discharge of 125 m3/s, which was the second lowest discharge modeled. At this discharge, all of <br />50