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<br />EM 1110-2.1416 <br />15 Oct 93 <br /> <br />Tr = hydrograph time of rise <br />So = equilibrium energy slope (or bottom slope for <br />channel of regular cross section) <br />Uo = average velocity <br />do = average flow depth <br />g = acceleration of gravity <br /> <br />b. Data requirements. These depend on the nature <br />of the method and are described in the sections which <br />follow and in Appendix D. In general, hydraulic models <br />require channel geometry, boundary roughness, the initial <br />state of the water in the channel, and an upstream flow <br />hydrograph. <br /> <br />(1) An upstream boundary condition with its time <br />variation, such as a discharge or depth hydrograph, must <br />be specified, as must be the tributary inflows or oulflows. <br />In the special case of supercritical flow at the upstream <br />end of the reach, both depth and discharge must be given <br />to a dynamic wave model. <br /> <br />(2) With the dynamic wave and diffusion models, <br />either a depth or discharge hydrograph is required at the <br />downstream end. In the special case of supercritical flow <br />at the outlet (dynamic wave model), no downstream <br />boundary condition can be given. <br /> <br />(3) No downstream condition can be given to the <br />kinematic wave model, nor to any of the hydrologic <br />models, as they all employ "marching" solutions, pro- <br />gressing from upstream to downstream. <br /> <br />5-16. Musklngum-Cunge Model <br /> <br />While the origin of this model is the Muskingum method. <br />a hydrologic technique, its theoretical basis and applica- <br />tion, typically to a large number of subreaches, suggest <br />that its classification be as a hydraulic method. As such, <br />it is a subset of the diffusion approach; the additional <br />assumption, linearization about normal depth at the local <br />discharge, leads 10 problems with accuracy at low values <br />of bottom slope and precludes analysis of flows in which <br />backwater effects play a role. Its advantages over the <br />diffusion approach are not known at this time; compari- <br />sons might prove it to be a more robust model. <br /> <br />5-17. Hydrologic Routing Schemes <br /> <br />Hydrologic routing focuses on the study reach as a <br />whole; there is still need for two equations 10 solve for <br />the two related variables, water surface elevation and <br />discharge, even if these are required at just one location. <br /> <br />5-30 <br /> <br />The principle of mass conservation supplies one of the <br />required equations but, instead of applying the momen- <br />tum equation in the interior of the flow. a different the0- <br />retical or empirical relation provides the second equation. <br />A summary discussion is presented below. <br /> <br />e <br /> <br />a. Average-lag methods. Two significant features of <br />flood hydrographs have long been observed in many <br />rivers. Reflecting the wave-like character of flood <br />behavior, hydrographs at successive stations are displaced <br />in time; peaks, for example, occur later at each succes- <br />sive downstream station. In other words, downstream <br />hydrographs lag upstream hydrographs. The second <br />observation is that, usually, hydrograph peaks exhibit <br />subsidence; that is, a decrease in peak value with dis- <br />tance downstream if there is no significant tributary <br />inflow. <br /> <br />(1) Such behavior is observed in the results of the <br />so-called average-lag methods, empirical techniques <br />based on averages of inflow hydrograph values lagged in <br />time. Averages of groups of hydrograph values are <br />always less than the largest of the group unless all mem- <br />bers of the group are equal; in particular, the average of <br />values in the vicinity of the peak will be less than the <br />peak itself. Ffe!:dom in choosing the time spacing of <br />points on the inflow hydrograph, the number of points 10 <br />inclode in the average, the weighting coefficients defin- <br />ing too average, the number and length of subreaches to <br />which to successively apply the technique, and the travel <br />time for the hydrograph in each subreach; i.e., the <br />amount of time to lag the hydrograph, often provides <br />enough flexibility 10 allow a match of lagged average <br />reach-oulflow hydrographs with observed ones in a cali- <br />bration event. Many years of familiarity with a reach of <br />river and with the observed hydrographs can facilitate <br />choosing the parameters of such a method for a reason- <br />ably good fit of computed and measured hydrographs, <br />but satisfactory routing under different circumstances <br />would have to be considered fortuitous. There are many <br />ways in which hydrograph values can be averaged and <br />lagged. There is no theoretical reason to favor one over <br />another. <br /> <br />e <br /> <br />b. Progressive average-lag method. This technique <br />as found in EM 1110-2-1408 also known as Straddle- <br />Stagger (U.S. Army Corps of Engineers 19903), is the <br />most empirical of these methods. It provides hydro- <br />graphs which exhibit subsidence and time lag, and these <br />can often be made 10 match observed hydrographs <br />through adjustment of the arithmetic parameters of the <br />method. <br /> <br />e <br />