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The second thing to note in these figures is that there was very little sediment coarser <br />than sand (D > 2 mm) caught in the traps in years when the peak discharge did not exceed -300 <br />m3/s. This is approximately the flow level that was recommended for producing initial motion of <br />the bed material [Pitlick and Cress, 2000]. The presence of pebbles and fine gravel in samples <br />taken near the peak in 1998 indicates that portions of the bed surface were indeed mobilized <br />during the period of high flow that year. These sizes are not as common in samples collected in <br />subsequent years, suggesting that, at flows less than -300 mils, most of the bed surface remains <br />immobile, as predicted. However, in addition, the data clearly show that even during periods of <br />low flow, the Colorado River continues to transport fine-medium sand (0.1 < D < 0.5 mm). In a <br />general long-term sense, this has probably always been the case; however, with streamflows now <br />regulated, there are concerns that the build up of fine sediment on the bed of Colorado River will <br />impair biological productivity [Osmundson'et al., 2002]. Thus, in addition to moving coarse <br />sediment on the bed surface, another management goal might be to augment flows on the <br />recessional limb of the hydrograph to keep fine-medium sand in suspension over the most <br />productive and important habitats (riffles). The criterion for suspension is based on an empirical <br />relation for estimating the settling velocity, ws , of natural particles in water as a function of grain <br />size and grain shape [Dietrich, 1982]. When the local fluid shear velocity, u> _ (ghS,)"', exceeds <br />the settling velocity of a given particle size, u< > ws, then those sizes should be transported in <br />suspension; otherwise they should move as bed load. Using Dietrich's [1982] relations for <br />quartz-density sediment with a shape factor or 0.7, the fall velocity for medium sand, D = 0.5 <br />mm, is calculated to be ws = 7 cm/s. Based on results from flow modeling in the reach near RM <br />176 (discussed in the next section), a discharge of 125 m3/s should be sufficient to keep particles <br />finer than 0.5 mm in suspension over riffles. <br />44