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a) <br />100.0 <br />98.0 <br />c <br />0 <br />m 96.0 <br />m <br />w <br />94.0 <br />92.0 <br />0 <br />b) <br />101.0 <br />99.0 <br />s <br />97.0 <br />c <br />O <br />R <br />95.0 <br />W <br />93.0 <br />91.0 <br />RKM 150 <br /> <br />. A ------ .----5 ----------- ----------A ------------ A -------- .-A..---.....-I <br />100 200 300 400 500 <br />Distance (m) <br />RKM 106 <br />---A ------------ A----------- A ----------- a----------- o........... A----------- I <br />-.--o-------0------o------0------o-----o-----+ <br />0 100 200 300 400 500 600 700 <br />Distance (m) <br />Figure 24. Bed and water surface elevations in reaches near (a) RKM 150 and (b) RKM 106. <br />In deriving the relations between Q and r' for these sites, we obtained some unexpected results. If <br />we formulate the dimensionless shear stress using the observed depth, slope and D50, we obtain <br />values of f that are low in comparison to what might be expected for the conditions. For example, <br />measurements at RKM 150 during a near-bankfull discharge of 1229 m3/s give a reach-average f <br />of 0.031 (Fig. 25a), which is only slightly above the assumed threshold for initial motion (0.030), <br />and well below the value expected for bankfull flow. Similarly, observations at RKM 106 during an <br />overbank discharge of 1456 m3/s give a reach-average f of 0.029 (Fig. 25b). These results imply <br />that bankfull flows in the lower reaches are barely capable of transporting coarse sediment, <br />assuming a threshold for motion of f = 0.030. That situation seems very unlikely, and it is clearly <br />not supported by field evidence. There are three possible explanations for this discrepancy: (i) <br />these two sites are not representative of the river as a whole; (ii) the measured grain sizes are not <br />representative of the reach; or (iii) the assumed value of 0.030 for the critical f is not appropriate <br />35