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Results of Groundwater Pumping Tests - 152 East 11 th Street, Tracy Page 12 <br /> Early-jime Data <br /> As noted previously, although the pumping tests performed on January 18th 1994, were <br /> adversely affected by intermittent freezing of the pump under the adverse weather <br /> conditions, useful early-time data was obtained from those tests through use of the <br /> electronic data logger and pressure transducer array Specifically, when Well NAV 6 was <br /> first pumped, good early-time data in the first minutes after the pump was started were <br /> obtained with drawdowns recorded at closely spaced intervals These data are plotted on <br /> Figure 10 <br /> That Figure shows that there is a distinct change in slope of the drawdown versus <br /> logarithm of time plot at 0 18 min after the pump was started Prior to that time, the plot <br /> is relatively steep and equates to a computed transmissivity of 864 gpolft Thereafter, the <br /> slope flattens and yields a computed transrrussivity of 3,895 gpolft which is in good <br /> agreement with the transmissivity of 4,324 gpolft , which was derived for the aquifer from <br /> the longer duration test that was performed on December 28th 1993 (See Figure 8 ) <br /> The bi-modal nature of the time-drawdown plot on Figure 10 is characteristic of early- <br /> time plots for wells where the time-drawdown relationship is initially dominated by <br /> evacuation of water from within the casing and only later by the hydraulic properties of <br /> the aquifer This phenomenon is known as the casing effect However, such bi-modal plots <br /> can also be produced in aquifers that are being recharged, or there is some boundary effect <br /> due to hydrostratigraphic variations within the zone of influence of the pumped well <br /> To check that the slope change of the seen on Figure 10 can be attributed to the casing <br /> effect, Schafer's (1978) procedure was used to estimate the duration of the casing effect <br /> using the equation <br /> Time (in Min ) after which the Casing Effect is Negligible, t, = 0 6 (dC2 - dp2) s / Q <br /> where <br /> Q = Steady State Pump Discharge Flow Rate (in GPM) <br /> dc = Inside Diameter of Well Casing (in in ), and <br /> dp = Outside Diameter of Pump Riser Line (in in ) <br /> For well NAV 6 the internal diameter of the casing is 1 78 in and the outside diameter of <br /> the piping installed in the well to evacuate the water was approximately 1 in Applying <br /> these and the other applicable parameter values to solve the above equation iterivly <br /> produced an estimate for to of 0 48 min which is close to the time at which the slope of <br /> the data plotted on Figure 10 changes This confirms the assumption that the very early <br /> drawdown data shown on the figure is influenced by the casing effect but that drawdown <br />