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<br />e <br /> <br />~ <br />. <br /> <br />. <br /> <br />. <br />. <br /> <br />e <br /> <br />:. <br /> <br />e <br /> <br />U.S. Department of Transporation 1989). Commonly <br />used in the Corps of Engineers is RMA-2 (King 1988) <br />which is the hydraulics module of the T ABS-2 modeling <br />system (Thomas and McAnally 1985). Synopses of these <br />and other programs are presented in HEC (U.S. Anny <br />Corps of Engineers 1982b). RMA-2 solves the vertically <br />(i.e., depth) averaged version of equations 4-1 to 4-4; <br />written as shown below. <br /> <br />Momentum equations: <br /> <br />hi + ~ + v~ + g~ + g~ <br /> <br />(4-5) <br /> <br />hE.xx <flu <br />P ax2 <br /> <br />hE.xy <flu <br />- -- + Sft + tx <br />P ay2 <br /> <br />~ 0 <br /> <br />~ + ~ + hdv + hila + ~ah <br />at ax v/iV g= g <br />y ay <br /> <br />hEyx <flv hE.yy <flv S ~ 0 <br />P ax2 -Pily2 + 1'Y +ty <br /> <br />(4-6) <br /> <br />Continuity equation: <br /> <br />ah + iJ(hu) + a(hv) ~ 0 <br />dtdXT <br /> <br />(4-7) <br /> <br />where <br /> <br />x ,y = the horizontal coordinate directions. <br />u,v = velocity components in the x and y <br />directions, respeclively. <br />t = time. <br />g = the acceleration due to gravity. <br />a = the bottom elevation. <br />h = the depth. <br />P = fluid density. <br />Ex:<' Exy, etc. = the turbulent exchange coefficients which <br />describe the diffusion of momentum in <br />the direction of the first subscript to that <br />of the second subscript. <br />Slx'SIY = terms for the nonlinear Manning or <br />Chezy representation of bottom friction. <br />'U, 't)' = terms representing boundary shear stresses <br />other than botlom friction (e.g., wind), <br />these terms also include the Coriolis <br />effect. <br /> <br />EM 1110-2-1416 <br />1S Oct 93 <br /> <br />4-8. Data Requirements <br /> <br />It is useful to think of "data" in three categories: <br />analysis input data, calibration data, and validation or <br />confirmation data, These categories are useful when <br />identifying data requirements for both physical and <br />numerical models. <br /> <br />a. Analysis input data. Analysis input data are those <br />items required 10 operate the model. They consist of a <br />geometric description of the study area (e.g., cross sec- <br />tions in one-dimension, contour maps, or a digital terrain <br />model for twlHlimensions), flow 10 be analyzed (a single <br />discharge for steady flow, or a hydrograph for unsteady <br />flow), other boundary conditions such as stages or rating <br />curves, and various coefficients that approximate the <br />effects of friction and turbulence. Of these, the geo- <br />metric description of the study area is usually the most <br />time consuming 10 develop and schematize; it is, how- <br />ever, not necessarily the most important data in terms of <br />simulation accuracy (U.S. Anny Corps of Engineers <br />1986). The density (i.e. resolution) and accuracy <br />required of the flow and geometric data are governed, <br />fundamentally, by the study purpose, not the analysis <br />technique (Cunge et al. 1980). <br /> <br />b. Calibration data. Calibration data consist of field <br />observations that are used to evaluate the performance of <br />a model and adjust the coefficients 10 improve its perfor- <br />mance, if necessary. "Performance" is a qualitative, or <br />subjective, measure of the degree to which the model <br />faithfully reproduces the field observations. This mea- <br />sure is applied by the engineer performing the study and <br />documented by means of the reporting process. The <br />complexities of river hydraulics do not allow the selling <br />of objective criteria to measure the accuracy of calibra- <br />tinn. Whether the model's performance is acceptable <br />depends on study objectives, sensitivity of study out- <br />comes 10 model results, and reliability of field data. <br /> <br />(I) The weight given 10 the performance of a model <br />with regard to different hydraulic variables, such as water <br />surface elevation or velocity, will vary with study objec- <br />tives, data availability and reliability, and the judgment of <br />the engineer. For example, floodway studies focus on <br />accurate computation of the water surface elevation while <br />constituent transport studies require accurate reproduction <br />of velocity, water discharge, and mixing. Surrogate data <br />should be used with caution. For example, if the study <br />objectives require the prediction of discharge, prototype <br />discharge should be measured for calibration rather than <br />derived from a rating curve. <br /> <br />4-5 <br />