Laserfiche WebLink
PITLICK AND CRESS: DOWNSTREAM CHANGES IN CHANNEL GEOMETRY 34 - 5 <br />1600 ,. ... .._ <br />15001 <br />1400 <br />I' <br />m <br />i <br />1300 <br />w ,. <br />12001 <br />1100 <br />-- RD ------ ? 6G 151N- _. tHNd... (------ Rki°. ?_ PINY ? ... CK°, 017 4 •' q8': hiY <br />350 300 250 240 150 100 <br />Distance Above Green River Confluence (km) <br />Figure 3. Longitudinal profile of the Colorado River between approximately Rifle, Colorado, and <br />Moab, Utah. The shaded lines indicate boundaries of reaches listed in Table 1. <br />DeBeque Canyon, Westwater Canyon and Professor Valley. <br />The first of these is caused by a series of three low-head <br />diversion dams which divert water into the Grand Junction <br />area. These dams alter the profile but do not reflect natural <br />processes. The breaks in slope through Westwater Canyon <br />and Professor Valley are related to local geologic and <br />tectonic processes. The segments in between these points <br />define smooth profiles, which are not strongly influenced by <br />transitions in reach type (alluvial to quasi-alluvial) or by <br />junctions with tributaries. The segment between DeBeque <br />Canyon (rkm 300) and Westwater Canyon (rkm 205) for <br />example, includes a major tributary, the Gunnison River at <br />rkm 274, and a transition in reach type at rkm 245. Neither of <br />these features appears to affect the profile in a strong way. <br />Elsewhere we observe similar trends, indicating that tran- <br />sitions between hard and soft sedimentary rocks have little <br />influence on the overall form of the longitudinal profile. <br />Similar to Rice and Church [2001 ], we find that the concave <br />segments of the profile are better fit by quadratic functions <br />than exponential functions. <br />4.2. Bed Material <br />[16] The bed material of this segment of the Colorado <br />River grades from cobbles and large gravels in the upper <br />reaches to medium gravels in the lower reaches. Plots of <br />specific percentiles of the surface grain-size distributions <br />(D84, D50i and D76) define a weak trend of downstream <br />fining (Figure 4). Locally high values in two of the lower <br />reaches (Professor Valley and Big Bend) skew the data <br />somewhat, but even with these values excluded, the surface <br />sediment fines at relatively slow rates. The trend lines <br />shown in Figure 4 (and subsequent figures) are fitted <br />exponential relations, In y = In a + bx, where In a is the y <br />intercept, b is the slope of the line, and x is the distance, <br />measured upstream with respect to the Green River (rkm 0). <br />In this case the coefficient a represents the grain size atx= 0, <br />and b represents the rate of downstream fining. These <br />values are listed in Table 3, along with relevant parameters <br />for the subsurface sediment, channel morphology and shear <br />stress. Comparison of the values of b for the surface <br />percentiles indicates that large and small sizes fine down- <br />stream at about the same rate (Table 3). In comparison to <br />trends reported in other studies [Knighton, 1998; Rice, <br />1999; Gomez et al., 2001], the rate of surface-fining in. <br />the Colorado River is relatively weak. In this case, surface <br />particle sizes change slowly downstream because coarse <br />material is continually supplied from local sources such as <br />ephemeral tributaries, terraces, and valley side-slopes. Input <br />from these sources is not large enough to overwhelm <br />downstream trends, but apparently sufficient to replenish <br />coarse material worn down by abrasion. <br />[17] A close inspection of the data in Figure 4 suggests <br />that the rate of downstream fining within several individual <br />segments is higher than the overall trend. Stronger fining is <br />apparent in the reach between DeBeque Canyon and West- <br />water Canyon (rkm 300-200), and in the reach below <br />Professor Valley (rkm 130-100). To evaluate the impor- <br />tance of these differences, we separated the data into four <br />segments bounded by the breaks in slope discussed pre- <br />viously. For each segment we derived separate exponential <br />relations for the surface D 0 (Table 4) (relations for the <br />bank-full width, depth, shear stress and Shields stress were <br />also derived, but, for the moment, we focus only on the <br />downstream trends in surface D50). The results listed in <br />300 <br />E <br />33 <br />1 D ....,.. .-..... <br />400 350 300 2507 200 150 100 <br />Distance (km) <br />Figure 4. Downstream trends in percentiles of the surface (pavement) grain size distribution.