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<br />TOPPfNG ET AL: COLORADO RIVER SEDIMENT TRANSPORT, 2 <br /> <br />563 <br /> <br />10 <br /> <br />RIVER MILE 28.5 <br /> <br />100 <br /> <br />lJl <br />~ <br />o <br />~ <br />;; <br />;;:: <br />* <br /> <br /> <br /> <br />0.1 <br /> <br />0.01 <br /> <br />0.001 <br /> <br />0.05 <br /> <br />0.1 <br /> <br />-0- 3-98 (0.59 nm) <br />---.- 8-68 (0.46 mm) <br />-lIl- 5-99 (o... nwn) <br /> <br />0.5 <br /> <br />1.0 <br /> <br />20 <br /> <br /> 100 <br />lJl 10 SECONDARY MODE <br />~ \ <br />0 <br />I!l <br />;; 0.1 <br />;;:: --0-- 3-98 (0.45 mm) <br />.. 0.01 --+- 9-98 (0..... nvn) <br /> -lIl- 5-99 (0.32 mm) <br /> 0.001 <br /> 0.05 0.1 0.2 0.5 1.0 2.0 <br /> GRAIN SIZE (nm) <br /> 100 RIVER MILE 50.1 <br />~ 10 -<>- 3-118 (0.32 mm) <br />__.... (0.33 mm) <br /> -lIl- 5-99 (0.42 mm) <br />" SECOND~Y MODE <br />I!l <br />;; 0.1 <br />;;:: <br />* 0.01 <br /> 0.001 <br /> 0.05 0.1 0.2 0.5 1.0 2.0 <br /> GRAIN SIZE (11lTl) <br /> 100 <br />~ 10 -<>- 3-.. (0.43 mm) <br />__"98 (0.33 mm) <br />" -lIl- 5-99 (0.38 mm) <br />w <br />N <br /><ii 0.1 <br />;;:: <br />* 0.01 <br /> 0.001 <br /> 0.05 0.1 0.2 0.5 1.0 2.0 <br /> GRAIN SIZE (nwn) <br /> <br /> <br /> <br />Figure 14. (continued) <br /> <br />where 1} is the elevation of the bed, Cb is the concentration of <br />sediment in the bed. VI" is the volume of sediment in suspen- <br />sion, and Q. is the flux of sediment. <br />Changes in the volume of sediment in suspension with re. <br />spectto time (~V,/~I) are driven primarily by changes in the <br />boundary shear stress at a given location over time. Colby <br />(1964] demonstrated that in a typical sand-bedded river, the <br />magnitude of bed scour and fill related to temporal changes in <br />the volume of suspended sediment during a flood (i.e., ~ V,I al) <br />is small. As noted by Rubin and Hunter (19821, the volume of <br />sediment available for deposition in response to iJVsliJl is <br />limited to the volume of sediment in transport over the depo- <br />sitional site on the bed. In contrast, when the volume of sed- <br />iment in transport decreases in the downstream direction, the <br />volume of sediment availa.ble for deposition includes all of the <br />upstream sediment in transport. Thus, in most situations, the <br />portion of scour and fill driven by V . Qs dominates over the <br />portion of scour and fill driven by aVslat. Indeed, in {he case <br /> <br />of the 1996 Grand Canyon flood experiment, only 1 cm of bed <br />scour althe Grand Canyon cableway would be needed to equal <br />the measured increase in the unit volume of sediment in sus- <br />pension during the rising limb of the flood. However, while this <br />maximum of 1 ern of bed scour could have occurred in re- <br />sponse to ~ V,I ~I during the rising limb of the flood, the bed at <br />the Grand Canyon cableway aggraded by 0.5 m in response to <br />V'Q,. <br />Divergence in the flux of sediment (V ' Q,l can be driven by <br />either reach-geometric effects, changes in the magnitude of the <br />upstream sediment supply, or both. For example, given a con- <br />stant upstream supply of sediment, streamwise divergence in <br />the flux of sediment at a cross section can be caused purely by <br />reach-geometric effects if, given a change in water-sudace <br />stage, the sediment-transport rate at that cross section in- <br />creases faster than the sediment-transport rate at the cross <br />section ups[ream. Conversely, a decrease in the upstream sup- <br />ply of sediment will also rcsuh in streamwise divergence in the <br />