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24 <br /> represent the permeability of an approximately 2 ft. thick fracture zone <br /> P P Y PP Y <br /> and is on the order of 10,000 times greater than the permeability measured <br /> on core plugs (Table 1 ). The storage coefficients shown in Table 2 are <br /> typical values for thin, well confined aquifers. <br /> No bedrock pumping tests were conducted at the Allen Mine and there <br /> i is , therefore, no direct way to compare coal seam permabilities at the two <br /> locations. However, it is possible to mathematically estimate inflows to <br /> the Maxwell Mine using the hydraulic properties discussed above and, by <br /> comparing with measured inflows at the Allen, establish some insight to the <br /> relative magnitudes of the controlling hydraulic properties at the two <br /> sites. <br /> Mathematical Estimate of Maxwell Mine Inflows <br /> The plan-view geometry of the Maxwell Mine will be complex, both during <br /> and after mining, and the changing geometry will affect the inflows to the <br /> mine. However, the advance of the mine and the precise geometry at a <br /> particular time consitute second-order considerations; the length of peri- <br /> meter separating the mine workings from the undisturbed ground being the <br /> most important aspect. A simple model whereby the total inflow is calcu- <br /> lated as the product of the length of perimeter and the inflow at points on <br /> the perimeter, obtained by assuming planar flow normal to the perimeter, <br /> retains the effects of first order importance. Flow to the mine is derived <br /> from storage in the water-bearing zones and is transmitted to the mine <br /> primarily through the undisturbed coal seam. <br /> Figure 6 is a schematic representation of the flow to the face at a <br /> particular point on the perimeter. The steady state distribution of drawdown <br /> is given by <br /> s = s o e x p ( x ) <br /> where s = drawdown at a point located a distance x from the face <br /> so = drawdown at the face <br /> 1 <br />