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<br />e <br /> <br />~ <br /> <br />, <br /> <br />.. <br /> <br />e <br /> <br />.. <br /> <br />'. <br /> <br />e <br /> <br />(1) The reach is treated as a whole; subreach length <br />equals reach length. Equal weight is given 10 the <br />inflowing hydrograph values in determining their <br />average. The time period over which averaging occurs is <br />centered on the inflow value being routed; i.e., the one at <br />a lag-time duration earlier than the time pertinent 10 the <br />outflow hydrograph value. The constant time interval <br />used to define the inflow hydrograph, the number of <br />points used for averaging, and the lag time (outflow <br />value time minus routed inflow value time, expressed as <br />an integer number of time intervals) are chosen by trial <br />and error for a best fit with observations. <br /> <br />(2) The hope in using this method is that the <br />storagelhydrograph relation that exists for the reach in <br />the calibration event is reflected in the arithmetic param- <br />eters determined, and that these will continue 10 be valid. <br />for the subject event. The lack of any theoretical basis <br />for this hope makes the method unreasonable rather than <br />approximate. The term approximate suggests that there <br />is some control over the amount of error. But, in princi- <br />ple, the error in the computed subsidence for the subject <br />event could be zero, plus or minus a hundred percent or <br />more. Only if a series of calibration events lead to about <br />the same parameter values in each case could one reason- <br />ably suppose that a subject event in the same reach with <br />about the same inflow hydrograph as the calibration <br />events, calculated with those values of parameters, would <br />yield an outflow hydrograph of about the same accuracy <br />as the calibration events. In general, the method is not <br />recommended. <br /> <br />c. Successive average-lag method. In this technique <br />(EM 1110-2-1408 19(0), also known as the Tatum <br />Method, each ordinate of the outflow hydrograph for a <br />subreach is the numerical average of the routed inflow <br />value and the preceding ordinate in the hydrograph. The <br />ordinates of the inflow hydrograph are separated by <br />constant time intervals, Ll.t, a parameter of the method. <br />Subreach length is defined as the distance traveled by the <br />flood wave in a time interval Ll.l/2, taken as the lag time. <br />The outflow hydrograph for a subreach constitutes the <br />inflow hydrograph for the next subreach, for which the <br />procedure is repeated. <br /> <br />(I) Additional subreaches are introduced until the <br />outflow for the subject reach bas been determined. The <br />number of subreaches constitutes another parameter of <br />the method. The parameter values are chosen for a best <br />fit with calibration hydrographs. <br /> <br />EM 1110-2.1416 <br />15 Oct 93 <br /> <br />(2) A physical interpretation of the Tatum Method <br />exists; it corresponds to a linear Modified Puis technique <br />in which subreach storage is directly proportional to <br />subreach outflow with the constant of proportionality K = <br />Ll.l!2. Nonetheless, the method, like Progressive Average- <br />Lag, must be considered empirical, and is not generally <br />recommended. <br /> <br />d. Modified Puis. This approach is more rational <br />than the average-lag methods, because it strives 10 solve <br />the mass-conservation relationship (equation 5-2) by <br />providing a second, storage versus flow, relation neces- <br />sary 10 close the system. <br /> <br />(I) The method is characterized by a far-reaching <br />physical assumption which, unfortunately, is often not <br />warranted in rivers. The required slorage versus flow <br />relation stems from the assumption that there exists a <br />unique relatinnship between storage in the reach and <br />outflow from the reach. It is further assumed that this <br />relationship can be found for the reach, either theoreti- <br />cally or empirically from past events; and that, once <br />determined, applies to the study event. The mathematical <br />form of the relationship is not important, a graph or table <br />of numbers will suffice. <br /> <br />(2) An empirical relation can be found by measuring <br />discharges as they vary with time during a calibration <br />flood event at the inlet and outlet of the reach and apply- <br />ing the volume-conservation principle, (Equation 5-2). <br />To the extent that tributary flow is accounted for, the <br />relationship is valid for the event for which the informa- <br />tion was recorded. To the extent that the relationship <br />will continue to be valid for another event, or a different <br />inflow hydrograph, it can be successfully used 10 predict <br />outflow hydrographs for that event <br /> <br />(3) A storage-outflow relation can be easily devised <br />for a channel which is so large that the water surface <br />remains level during the event 10 be simulated (a reser- <br />voir or "level pool") and if a discharge coefficient, the0- <br />retical or empirical, is available for the outlet. This is <br />the physical circumstance for which the basic assumption <br />of the Modified Puis method is valid. <br /> <br />(4) Hypothetical relationships between storage and <br />outflow are sometimes derived for rivers from steady <br />flow computations. Steady water surface profiles and, <br />hence, water volumes, are computed in the reach for a <br />sequence of discharges (outflows). The resulting table of <br /> <br />5-31 <br />