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<br />". <br /> <br />l04i-- "--- <br /> <br />-- T-- --- ----- <br /> <br />--,--- <br /> <br /> <br />j--- <br /> <br />~-----+ --- <br /> <br />- - \ ' _l------1~5Jl--- <br />B6 -t-'Xs~8~-----~_XS~~,--- <br />B4-i---:-~::---~- ~ ---- ~----.----- <br />o 500 1(00 1500 <br />HORIZONTAl DISTANCE (ft) <br /> <br />= <br /> <br />FlGUR E 7. Bed profile and energy grade line pro- <br />files for discharges between 500 and 10,000 cfs in <br />the right branch channel, RM 16.5, Yampa River. <br />Tertiary bar or riffle locations are also shown. <br /> <br />stress to mobilize the bed material; when <br />7*' > 1, particle mobilization is indicated. <br />The effect of the riffles or tertiary bars <br />on the local hydraulic conditions in the <br />study reach can be seen in the velocity and <br />dimensionless grain shear stress profiles <br />for the right channel. At all discharges the <br />riffles or tertiary bars are zones of locally <br />higher velocity, and in general the profiles <br />indicate that velocity increases with dis- <br />charge at all locations (Figure 6). This is <br />especially true in the pool upstream of the <br />midchannel bar (upstream of cross section <br />5.1) where at low flow (500 cis) the velocity <br />is < 1 it/sec and at high discharge (10,000 <br />cis) it is >5 ft/sec. In contrast, depending <br />on location, the dimensionless grain shear <br />stress is greatest at lower discharges (Fig- <br />ure 9). At cross section 0.8 the maximum <br />dimensionless grain shear stress occurs at <br />500 cis, at cross sections 2.7 and 5.1 it occurs <br />at 1,200 cis. Without exception, in both <br />branch channels, the highest dimension- <br />less grain shear stresses occur at the riffles <br /> <br />::r--J--~----r-~- i -_____r--- <br /> <br />, I <br />100.. . !-i~...-'. <br /> <br />I ~~~i~~~E~: <br />:t----!J\.5:-=~~~~1~~5.=~~~I~ ~ ~~ I <br /> <br />84--<- ___ _ _J_ ----~--- <br />o SCXl 1aD 1'5ID 200) 2SXl 3Co:) <br />HORIZONTAl DISTANCE (ft) <br /> <br />FIGURE 8. Bed profile and energy grade line pro- <br />files for discharges between 500 and 10,000 cfs in <br />the left branch channel, RM 16.5, Yampa River. Ter- <br />tiary bar or riffle locations are also shown., <br /> <br />~ 3_0T, --------. <br />~ I <br />~ 2,51-~----- <br />0::: _ ____, <br />t;) xso_a; <br />~ 2.0-j--- <br />r ! <br />(f) <br /> <br />~ '.5~__ <br /> <br />ill 10 I <br />:;i <br />o <br />~ 0.5 <br />UJ <br />::;; <br />is <br /> <br />XS2_7 <br /> <br />,(55.' I ---e-- lOOXlds <br /> <br />= 0 -~------t~_;: r <br /> <br /> <br />2500 <br /> <br />0.0 <br />o <br /> <br />soo <br /> <br />----I <br />1001 1500 2(0) 2SXl <br />HrnlZONT AL DISTANCE (ft) <br /> <br />FIGURE 9. Dimensionless grain shear stress (T.') <br />profiles for three discharges in the right branch <br />channel, RM 16.5, Yampa River. Tertiary bar or riffle <br />locations are also shown. When T.' > 1 bed material <br />is mobilized. <br /> <br />or tertiary bars at discharges less than <br />10,000 cis. Comparison of the velocity pro- <br />files (Figure 6) and dimensionless grain <br />shear stress profiles (Figure 9) for the three <br />riffles or tertiary bars in the right branch <br />channel demonstrates that average veloc- <br />ity alone does not adequately represent the <br />force applied to the bed material by the <br />range of flows that control the bar dynam- <br />lCS. <br /> <br />Spawning Habitat Identification <br /> <br />Analysis of the variations in dimension- <br />less grain shear stress (7*') over a range of <br />discharges at each of the riffles or tertiary <br />bars in the right branch channel provides <br />an explanation for the association between <br />the fish-capture sites and the riffles or ter- <br />tiary bars. Considering first the down- <br />stream riffle (Figure 3, cross section 0.8), <br />where the median grain size (050) is 68 mm <br />(2.7 in.), the dimensionless grain shear <br />stress (7*') falls below 1.0 (incipient mo- <br />tion) at discharges between 970 and 1,300 <br />cis depending on the value of 7 *c being <br />used (Figure 10). Dimensionless grain shear <br />stress reaches a maximum at this riffle at a <br />discharge of 800 cis when the hydraulic <br />gradient is steepest and decreases as dis- <br />charge increases and the riffle is drowned <br />out by increasing backwater (Figure 7). At <br />the time of the field sampling of the bed <br />material in 1991, when the discharge in <br />the river was about 1,200 cis, the bed ma- <br />terial in this riffle was not mobile. No fish <br />were captured in the associated down- <br />stream eddy formed by the convergence of <br /> <br />I M. D. Harvey et al. <br /> <br />123 II~ <br />