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<br />9 <br /> <br />where <br />V = mean flow velocity <br />y = flow depth <br />a, b, and c = coefficients determined by means of regression analysis <br /> <br />The regression coefficients are determined either from field data or by <br />generating data using the Meyer-Peter and M'~ller formula and Einstein's bed- <br />load function for bed-load and suspended-load discharges, respectively. The <br />model does not take into account changes in bed-material composition. <br /> <br />5. Numerical Scheme: <br /> <br />KUWASER first solves (2-7) and (2-9) for a spatially-varied, steady flow <br />by means of the first order Newton-Raphson method. Equations (2-7) and (2-9) <br />are combined to yield the following expression for the sole unknown, flow <br />depth at section 2, O2: <br /> <br />2 <br />Q2 a2 <br />aC2g" O2 <br /> <br />2 <br />411X Q2 <br />+ O2 - <br />2 a4 a6 <br />K1 + 2K1a302 + a502 <br />2 <br />alVl <br />+ a6~ + z2 - HI = 0 <br /> <br />.... (2-11) <br /> <br />where <br />Q2 = water discharge at section 2 <br />Kl = conveyance at section 1 <br />z2 = bed elevation at section 2 <br />aI, a2' a3' a4' a5' and a6 = regression coefficients determined from field <br />data <br /> <br />Note that effect i ve depth and wi dth, cross-sect i on area, conveyance, and <br />velocity-head correction factor are all expressed in terms of power functions <br />of the thalweg flow depth, O. Once the backwater calculation is co""leted, <br />sediment-transport rates at all cross sections are co""uted from (2-10). The <br />