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<br />flows including very small discharges, it became necessary to create artificial rectangular <br /> <br />channels at both ends of the modeled reaches. These artificial channels allow the model to <br /> <br />have stable boundary conditions that never go dry while still allowing for the modeling of <br /> <br />flows that would otherwise dry out elements at the inflow and outflow boundaries of the <br /> <br />mesh. HEC-RAS was used to develop stage discharge relationships for the artificial <br /> <br />rectangular channels. HEC-RAS output was also calibrated against known water surface <br /> <br />elevations to estimate a Mannings n for the channel, to determine the wetted perimeter at the' <br /> <br />highest modeled discharge for use in creating the mesh, and for evaluating wetted perimeter <br /> <br />(I-D) vs. wetted area (2-D) as stated in the objectives. <br /> <br />HEC-RAS is a I-D hydraulic flow model created by the Hydrologic Engineering <br /> <br />Center of the U.S. Army Corps of Engineers (Brunner, 1998), and is based on solution of the <br /> <br />one-dimensional energy equation (1). <br /> <br />O!;. <br /> <br />a V 2 a v2 <br />y. +z +~ = Y. +Z +--1..l..-+h <br />2 2 2g 1 1 2g e <br /> <br />(1) <br /> <br />where Yl'y2 = depth of water at cross. sections <br /> 21,22 = elevation at cross sections <br /> Vl,V2 = average velocities (total discharge/total flow area) <br /> al,a2 = velocity weighting coefficients <br /> g = gravitational acceleration <br /> he = energy head loss <br /> <br />h = LS + Ca2Vz2 _ al~2 <br />e f 2g 2g <br /> <br />(2) <br /> <br />'";' r i.;. <br /> <br />where L <br />Sf <br />C <br /> <br />= discharge weighted reach length <br />= representative friction slope between two gross se~.ti<?,ns <br />= expansion or contraction loss coeffiecient <br /> <br />Water surface profiles are computed from one cross section to the next by solving the <br /> <br />energy equation with an iterative procedure called the standard step method. The steady flow <br /> <br />22 <br />