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Last modified
11/23/2009 10:40:51 AM
Creation date
10/4/2006 10:26:20 PM
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Floodplain Documents
County
Statewide
Title
River Hydraulics
Date
10/15/1993
Prepared By
US Army Corps of Engineers
Floodplain - Doc Type
Educational/Technical/Reference Information
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<br />EM 1110-2-1416 <br />15 Oct 93 <br /> <br />are influenced by backwater. At these stations the rating <br />curve is modified not only by the shift but also by a <br />slope correction which is computed from the observed <br />fall to a downstream gage. Discharge records at a slope <br />station are seldom very good and should be used as <br />boundary conditions with caution. <br /> <br />(3) There are gaging stations whose records are not <br />very reliable. These are usually on streams with a flat <br />bed slope or a mobile boundary. At these locations, only <br />the actual flow measurements can be used with <br />confidence. <br /> <br />5-9. Calibration and Verification <br /> <br />When a model is calibrated, the parameters which control <br />the model's performance, primarily Manning's n and <br />reach storage, are determined. The key to a successful <br />calibration is to identify the troe values of the parameters <br />which control the system and not to use values that com- <br />pensate for shortcomings in the geometry and/or the <br />boundary conditions. Because unsteady flow models <br />reproduce the entire range of flows, they should be cali- <br />brated to reproduce both low and high flows. <br /> <br />a. Manning's n. In the unsteady flow models used <br />in the United States, the friction slope is generally mod- <br />eled using Manning's equation. Manning's n value <br />relates the roughoeSS of the stream boundary 10 the fric- <br />tion force exerted on the system. For most problems, an <br />initial estimate of Manning's n (it is only an educated <br />guess) is used at the start of the calibration. The initial <br />values are then adjusted to match observed stage data. <br />When no observed stage data exists, the estimated values <br />take on a greater importance since they are assumed 10 <br />be representative of the system. See Appendix D for <br />detailed information on selecting n values. <br /> <br />b. Calibration. Calibratinn of an unsteady flow <br />model is a four step process. In the first step the n val- <br />ues are adjusted to reproduce the maximum stages of an <br />event. The storage in the cross sections. is then adjusted, <br />if necessary, 10 improve timing and attenuation. In the <br />third step, the flow versus Manning's n relationship is <br />adjusted to reproduce both high and low flow event <br />stages. Finally, the model is fme tuned to reproduce a <br />longer period which should include the initial calibration <br />event. <br /> <br />(1) The initial calibration event should be one of the <br />larger events which are available in the time series. The <br /> <br />5-16 <br /> <br />purpose of this pbase is to adjust the initial n values 10 <br />match the crest of the event at all stations in the model. <br />Figure 5-12 shows the hydrographs for the Illinois River <br />at Havana after the initial calibration. Note that, <br />although the crest stage is approximately correct, the <br />timing of the hydrograph and the reproduction of low <br />flow are defICient. <br /> <br />e <br /> <br />(2) Total storage as defined by river cross sectinns <br />is almost always deficient. In natural rivers, the timing <br />of the hydrograph is determined by storage and the <br />dynamics of the flood wave. Timing can be adjusted by <br />modifying storage, friction, and distributinn of lateral <br />inflows. If the timing cannot be calibrated by reasonable <br />adjustment of these factors, then there is some other <br />problem, most likely an error in the cross sections. For <br />the Illinois River, which is confined by levees in the <br />reach near Havana, an increase in overbank storage of <br />about 20 percent yields the results shown in Figure 5-13; <br />an increase in storage of about 40 percent yields those <br />shown in Figure 5-14. Both changes are only minor <br />increases in storage area because the overbanks are con- <br />fined by levees. <br /> <br />. <br /> <br />.. <br /> <br />. <br /> <br />... <br /> <br />(3) By varying Manning's n with flow the reproduc- <br />tinn of stage is improved; see Figure 5-15. The model <br />still. does not reproduce the initial time steps, but the <br />disagreement is probably caused by the initial conditions. <br /> <br />e <br /> <br />(4) The final calibration consists of fine tuning the <br />flow-roughness relation and the adjustments in storage. <br />The event selected should be an extension of the event <br />chosen for the initial calibration. For the Dlinois River <br />example, the fmal calibration was performed for the <br />period from 15 Nov 1982 to 15 Sep 1983. The event <br />includes high flow and low flow and a second major <br />flood in May 1983. Figure 5-16 shows the reproduction <br />of stage at Havana during the period. The model param- <br />eters required only slight adjustment to better simulate <br />low flow. <br /> <br />. <br /> <br />c. Verification. The calibrated model should be <br />verified against two or more periods which include sig- <br />nificant events. The periods should be long, approaching <br />one year, so that seasonal effects can be detected. <br />Figure 5-17 shows the reproduction of the 1974 observed <br />data on the Illinois River. <br /> <br />. <br />. <br /> <br />e <br />
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