Laserfiche WebLink
Vs = 1n49 R2/s Si/2 (2) <br />where, <br />Vs = mean velocity of surface water <br />n = roughness coefficient, assumed to equal 0.035 <br />for all calculations <br />R = Hydraulic radius, equal to the conveyance area <br />A (width X mean depth), divided by the wetted <br />perimeter, (width + 2 X mean depth). For wide, <br />shallow channels, the hydraulic radius approxi- <br />imates the mean depth. <br />S = Energy gradient; for uniform flow assumed parallel <br />to hydraulic gradient. <br />From equations (1) and (2) it is seen that, <br />Va _ V2 n2 <br />S = K 2.22 R4~3 (3) <br />and <br />Va = Vs2 n2 K <br />2.2~T3 <br />(4) <br />It may be shown that the limit of equation (4), as R approaches <br />zero, is K. At small depths and velocities, fine sediment may deposit <br />in the interstices of the gravel, lowering the value of K, the perme- <br />ability. <br />Therefore, for a given slope and required apparent velocity, the <br />critical factor at low flow is maintaining sufficient shear stress to <br />prevent deposition of finer particles on the gravel. This critical <br />shear stress is defined as: <br />Tc = wRS (5) <br />where, <br />w =-unit weight of water - 62.4 lb/ft3 <br />R = Hydraulic radius <br />S = Energy gradient, assumed parallel to <br />hydraulic gradient <br />Survival rates of salmonid embryos, as a function of apparent <br />velocity, were found in Wickett (1958), Coble (1961), and Cloern (1976). <br />For a stipulated slope, K was calculated from equation (1) for each <br />apparent velocity listed. Terhune (1958) listed particle size distri- <br />15 <br />