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<br />00077'~ <br /> <br />~i? <br /> <br />fg} <br /> <br />The influence of the lateral shift in storage outside the plot boundaries <br />is quite evident in the mound cJ:oss sections from pond No.2 (fig. SA and B). <br />Under the pond, the observed mound (identified as OB) is closely appJ:oximated <br />by the theory based on the minimum V obtained from the well test (see table 1). <br />The cross sections approach the theoretical cross section'outside the plot <br />associated with the maximum estimated V. The same is evident, but to a much <br />lesser extent, at pond No. 1 (fig. 8e) where the relative change in void is <br />smaller, and the overriding effect of D is the main influence. In both compar- <br />isons, however, an estimate of the void outside the pond boundary is needed if <br />an acceptable theoretical estimate of the ground water mound height is to be <br />obtained. <br /> <br />Falling Hydrograph <br /> <br />A modificiation of equation 1 can be used to estimate the fall of the cen- <br />ter of our observed ground water mound if we assume it to have a disk shape <br />with idealized J:adius (a) and initial height (H). Equation 1 takes the form: <br /> <br />ho = H (l_e-a2/4C!t) (6) <br /> <br />We can assume that H equals the final observed height of the rise of the mound. <br />From this value, we can approximate a fJ:om the total volume of water storage in <br />the mound when spreading ceased, plus the water that dJ:ained from the vadose <br />zone beneath the plot during the period of observed fall. This was accomplished <br />as follows: <br /> <br />Let V ' '" the total volume of water metered on the 2-acre ponds <br />a <br /> (acre feet) <br /> Vi' '" volume of wateJ: in vadose zone at the beginning of <br /> spreading (acre feet) <br /> Vr' '" volume of wateJ: in vadose zone at end of spreading <br /> (acre feet)8 <br /> Vf' = volume of water in vadose zone at the end of observed <br /> fall (acre feet) <br /> V' effective mound volume (acre feet) <br /> <br />then the total volume of the mound plus that volume of water draining into it <br />during the fall is the effective mound volume: <br /> <br />V' = va' - (Vr' - Vi') + (vr' - Vf') = Va' - (Vf' - Vi') <br /> <br />where Vi', Vr', and Vf' were determined by averaging moisture profile observa- <br />tions in thJ:ee neutron access tubes in the pond area. <br />From Vi' (table 2) and the appropriate fil1ab1e void (V) (table 1), the <br />disk radius (a) at pond No. 1 equalled 894 feet and at pond No.2, 910 feet. <br />These values weJ:e used along with the aquifeJ: parameters from the pump test to <br />evaluate equations. The observed and theoretical hydrograph data were plotted <br />on figure 9. .The agJ:eement at pond No. 1 waS quite good with the apparent de- <br />viation being explained in part by the fact that the wetted depth (D = 16 feet) <br />used in the theoretical evaluation was low in comparison with the actual mound <br /> <br />8This expression would include the storage in the perched water table with <br />the vadose zone at pond No.2. <br /> <br />12 <br /> <br />~f~J!~it <br /> <br />q<-~-~:~-.~-:~-,-...:) <br /> <br /> <br />'-'.'. <br /> <br />:.".;: .-.: <br />.,...... <br /> <br />"""',"." <br />',".-.-" <br /> <br />'-J <br /> <br />-"....-... <br /> <br />-.-" <br /> <br />~> ?:-.->~:. <br />,'-;.' ~_.;.-..J <br /> <br />--..-, <br /> <br />,:<,:~,---,},:,-_::, -. <br /> <br />-'.': <br /> <br />'." .". <br /> <br />." -.- -., <br />'-.". -.-.'.- <br /> <br /> <br />~l'i~_~<<\!f~~(~~~~t~~t~~i~i\~~~j>~ <br />