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<br />566 <br /> <br />TOPPING ET AL: COLORADO RIVER SEDIMENT TRANSPORT, 2 <br /> <br />-WATER SURFACE <br />- BeD WITH EQUIUBAIUM UPSTREAM SAND SUPPLY <br />- - . BED wm-t DECREASING UPSTREAM SAND SUPPlY <br /> <br />w <br />'" <br />< <br />.... <br /><II <br /> <br /> <br />MAX. <br /> <br />------ <br /> <br />---- <br />--- <br />---- <br /> <br />0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0 <br />8) TIME NORMAUZED BY FLOOD DURATION <br /> <br />w <br />'" <br />< <br />.... <br /><II <br /> <br /> <br />--- <br />---- <br /> <br />----- <br />---- <br /> <br />0.0 0.1 0.2 0.3 0.4 0.6 0.6 0.7 0.8 0.9 1.0 <br />b) TIME NORlIAUZEO BY FlOOO DURATION <br /> <br />Figuft 17. ResulIs of calculations based on equation (I) for <br />cases where the upstream supply of sediment does not change <br />with time and decreases linearly with time during the cowse of <br />a flood for cross sections where (a) geometrically driven con- <br />vergence in the sediment flux occurs with increasing flow depth <br />and (1)) geometrically driven divergence in the sediment flux <br />occurs with increasing flow depth. <br /> <br />case of a decreasing upsiream supply of sediment, (I) maxi- <br />mum bed elevation will lead the flood peak at a cross section <br />where the bed aggrade5 with increasing water-swface stage <br />(Figure 17a), and (2) the time of minimum bed elevation will <br />lag the flood peak at a cross section wbere the bed SCOUTS with <br />increasing water-swface stage (Figure 17b). <br />If the assumption used in Figure 17 does not apply and the <br />timesca1e of bed-topographic adjustment is sqbstantial wiih <br />respect to the timescaIe of the rising limb of a flood, the effect <br />is to delay the time of either maximum or minimum bed ele- <br />vation. Therefore, in the first type of cross section (Figure 17a), <br />the time of maximum bed elevation does not ~ave to occur <br />prior to, but could occur either with or after, the time of a flood <br />peak. In the second type of cross section (Figures 17b) the time <br />of minimum bed elevation will still occur after the lime of a <br />flood peak, and the bed may still .ggrade during the receding <br />limb. Thus, in this case the effect of a slower response of the bed <br />topography to changing flow conditions produoes a result that <br />cannot be distinguished from the effect of sand supply limitation. <br />In summary. at a cross section that aggrades with increasing <br />water-surface stage, the observation that the time of maximum <br />bed elevation occurs prior to either the peak or the receding <br />limb of a flood indicates a decrease in the upstream supply of <br />sand during a flood (i.e., sand supply limitation). However, al <br />a cross section that scours with increasing water-surface stage, <br />the observation that the time of minimum bed elevation occurs <br />after the peak of a flood does not necessarily indicate the <br />presence of sand supply limitation. Therefore, because of the <br />strong control of reach geometry on bed topography and the <br />possibly delayed response of bed topography to changing flow <br />conditions, the best type of cross section to use in deducing the <br /> <br />presence of sand supply limitation is one tbat aggrades with <br />increasing water-surface stage (e.g., the Grand Canyon cable- <br />way cross section). <br />Observations made during the 1996 flood experiment sug- <br />gest that changes in bed elevation during floods in the Colo- <br />rado River in Grand Canyon are primarily driven by reach <br />geometry and only secondarily by depletion of the upstream <br />sand supply. Depletion of the upstream supply of sand does not <br />necessarily prevent bed aggradation when a strong streamwise <br />convergence exists in the boundary shear stress field. Measure- <br />menIs of suspended-sand concentration and bed grain size at <br />the Grand Canyon cableway during the 1996 flood indicate <br />that the upstream supply of sand was being depleted as early as <br />day 1 of the flood, 4 days before the bed stopped aggrading. <br />Depletion of the upstream sand supply therefore only bas the <br />effect of creating or modifying a lag between the time of a <br />flood peak and the lime of either maximum or minimum bed <br />elevation. At a cross section where convergence occurs in the <br />boundary shear stress. field with increasing flow, the time of <br />maximum bed elevation in a supply-limited case will occur <br />prior to that in a nOlHUpply-limited case; and, at a cross section <br />where divergence occurs in the boundary shear stress field with <br />increasing flow, the lime of minimum bed elevation in a supply- <br />limited case will occur after that in a non-supply-limited case. <br /> <br />6.2, Sediment Grain-Size Evolutioa <br /> <br />The concentration and grain size of sediment in suspension <br />is tightly coupled 10 the grain-size distribution of the bed. For <br />steady, uniform flow, and an upstream supply of sediment that <br />is in equilibrium with the flow conditions, the concentration of <br />each size class of sediment in suspension depends mainly on <br />(I) the proportion of the fine sediment on the bed composed <br />of that size class, (2) the settling velocity of that size class, and <br />(3) the median size of the fine sediment on the bed. In this <br />framework the grain-size distnbution of the bed is treated as <br />an independent variable. However, in riveTS in which the ilp- <br />stream supply of sediment is not in equilibrium with the flow <br />conditions, the grain-size distribution of the bed is a dependent <br />variable (as in either sediment-feed flumes or the Colorado <br />River) and evolves over time as a function of changes in the <br />sediment supply. Before adding thi6 degree of complexity to <br />the problem, it is useful to review the coupling between the <br />suspended and bed sediment in tbe Colorado River tbrough <br />solution of the foUowing equations for suspended-sediment <br />concentration derived for multiple size classes in steady, uni- <br />form flow and an upstream supply of sediment that is in equi- <br />librium with the flow conditions. <br />In steady, uniform flow, when the effects of bedfonns and <br />density stratification are excluded, <br /> <br />(C) (C ) [(a)(h-Z)]' <br />~ = ~ - - z<02h <br />1 - cJ J 1 - cJ" Z h - a - . <br /> <br />C ~mJ, ~ C ~mJJ (O~h)(:'~:) r <br /> <br />(2a) <br /> <br />'exp [ -p ~ (z - O.2hl] <br /> <br />These equations were derived using the two-part eddy viscosity <br />of Rnltray and MitswUl [1974]; see McLean [1992] for the basis <br />of the derivation. In 2, em is the volumetric concentration of <br />sediment in size class m I C s is the total concentration of sed- <br />iment in all size classes, z is the vertical dimension, h is the flow <br /> <br />Z > O.2h. (2b) <br />