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<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 />47 <br /> <br />Old Gauge <br />This site shows a general increase in reach averaged velocity, depth, <br />slope, and shear stress with discharge (Table 9). Figure 22 shows that at low <br />discharge theflow accelerates over a riffle at the downstream end of the site. <br />As the discharge increases, the discrepancy of velocity between cross-sections <br />evens out as the bed topography becomes drowned out and the water surface <br />slope becomes more uniform. The discharge for initial motion of the bed <br />material occurs near 525 cms (18,500 cfs) and significant motion occurs near <br />1,050 cms (37,000 cfs) (Fig. 22). These are approximately the 1.42 and 5.5 year <br />flood respectively. <br />New Gauge <br />At this site the reach averaged slope is steeper at low flow than at <br />moderate to high flows due to a riffle at the downstream end of the site. <br />Overall, however, the shear stress increases with discharge due to an increase <br />in depth (Table 10). Figure 23 illustrates how the water surface slope mimics <br />the bed topography at low flows, but again becomes more uniform as <br />discharge increases. 1?e average slope is steeper at this site than at the old <br />gauge site, so there is a higher shear stress for a given flow. Initial motion of <br />bed material occurs at a discharge near 275 cms (9,700 cfs), and significant <br />motion occurs at 875 cms (30,900 cfs) (Fig. 23). These flows have return periods <br />of 1.02 and 2.9 years respectively. <br />