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<br />I <br /> <br />Calibration of the Beaver Creek Valley Model <br /> <br />'J <br /> <br />Calibration of a digital ground-water model consists of entering known <br />~nd estimated input data, running the model for some historic period of <br />Istress, comparing modeled water levels to measured water levels, and then ad- <br />ljusting certain input data until the modeled and measured water levels ,com- <br />:pare within some acceptable limit of error. Typically, the boundary fluxes <br />'and historic "tresses are known and most adjustments of input data involve <br />it he storage coefficient and the transmissivity. In this study, however, due <br />;to a lack of data, boundary fluxes and historic stresses also were adjusted <br />Id' l'b' <br />I ur,ng ca I ration. <br />i <br />I Boundary fluxes were the first variables estimated for the Beaver Creek <br />:valley model. These boundary fluxes are the only source of "'ater into the <br />model, representing the flow of water through the alluvial valley from the <br />'south and from the sand dune areas to the east and west. The recharge to the <br />alluvial aquifer from the occasional flooding of Beaver Creek and recharge <br />:from intense precipi tation on the val ley floor were ignored for the average <br />'conditions being modeled. To determine the order of magnitude for estimated <br />:inflow, the possible recharge from the sand hill area was computed. If 3 in. <br />per year of precipitation were recharged--2.5 in. per year of recharge was <br />computed for Frenchman Creek basin, Nebraska, less than 100 mi east of this <br />site, where precipitation is about 75 percent greater but only one-third of <br />'the basin is sand dunes (Lappala, 1978)--over the approximately 200 mi2 of <br />'sand dunes, a total of about 44 ft3/s would be avai lable to enter the tl"O <br />illluvial valleys. <br />I <br />I The steady-state flux across the boundaries and into the stream channel <br />was computed for the water-table configurations in 1947 and 1978. A uniform <br />hydraulic-conductivity value was used for these computations. The initial <br />simulation, using a hydraulic conductivity of 500 ft/d, resulted in a bound- <br />ary flux and streamflow values that were much too large. Although no dis- <br />charge data were available for Beaver Creek, 25 ft3/s was estimated to be the <br />maximum possible average annual flow in 1947 and there was no flow in 1978. <br />Pumpage in 1947 was reported to total about 12,000 acre-ft, which converts to <br />about 16 ft3/s, and in 1978 pumping was assumed to be somewhat greater. On <br />the basis of these values, the estimate of hydraulic conductivity was ad- <br />Justed to about 90 ft/d. Using the water-table values of,1947, the flux at <br />each of the individual nodes along the boundary was computed; the sum was <br />21 ft3/s. The values estimated using the 1978 water-table configuration were <br />thought to be more accurate. This is because there was no flow in Beaver <br />Creek, so the hydrologic system is less complex and the hydraulic-head data <br />are affected by fewer external conditions. Also, the change in water levels <br />was smaller in 1978 than in 1947, so the hydrologic system was closer to a <br />steady-state condition. The sum of the fluxes using the 1978 water-table <br />values was 23 ft3/s. <br />! <br />i <br /> <br />L_ <br /> <br />" <br /> <br />46 <br /> <br />-----.:-~. <br />