Laserfiche WebLink
asci IU mo I y M itv No sy A r 4 ,/54 <br /> Figure 7 presents a view of the separating stream surfaces of all three water <br /> bodies in connection with the flow around a UVB The natural groundwater flow comes <br /> from the left side (In Figure 7b the three water bodies were artificially separated for <br /> clarification.) <br />' At the left side of Figure 7, the separating stream surface of the contaminated <br /> groundwater captured by the UVB can be seen In the center a water body is shown <br /> which consists of cleaned groundwater and shows the circulation flow around the UVB. <br /> At the right side of Figure 7, the separating stream surface of the cleaned groundwater <br /> flowing downstream is displayed The calculation has accounted for the following <br /> dimensionless parameters- Q/(Hlv) = 30, a/H = 0 25, and KH/K, = 5 The screen lengths <br />' at the bottom and top are the same- ar = as = a <br /> Diagrams for the Dimensioning of WB Installations <br /> Absence of Natural Groundwater Flow. At sites without natural groundwater flow, the <br /> sphere of influence (R) of a UVB is of special interest R is dependent on the anisotropy <br /> (horizontal over vertical hydraulic conductivity- KH/Kv), on the thickness (H) of the <br /> aquifer, and on the length of the screen sections ar and as at the top and bottom of the <br /> aquifer (see Fig 8) or the ratio a/H (when the same length of the screen section is used <br /> for both, then only a is referred to) Although R is mathematically mfinilf., it is, in <br /> practice, defined as the horizontal distance from the well axis to the farthest point at <br /> which circulation flow is still significant. Ina dimensionless description, R has been made <br /> dependent on the ratio QR/Q,where QR is that water quantity,which circulates within the <br /> distance R from the well. The ratio QR/Q, which is prescribed for practical reasons, <br /> describes the strength of a circulation flow at the distance R from the well. <br /> In Figure 9a, results are presented for ratios Qs/Q = 0 98 and 0.8 and for a = ar <br /> = as in a dimensionless diagram. The sphere of influence (R) is independent of the dis- <br /> charge through the well, but strongly dependent on the anisotropy KH/K,,. Within usual <br /> proportions, the length of the screen sections has only a small influence. For a UVB with <br />' separating plate and additional pump, a totally screened well casing should be avoided <br /> because of hydraulic shortcircuiting. <br /> Figure 9b presents a dimensionless diagram that describes the differences (eh) of <br /> the hydraulic heads between the top and bottom of a double-screened well through which <br /> ==H <br /> Ah =hT-he ( Or ; 0 - 2nr f vrdz <br />' hv,1zl z,H12 <br /> T <br />' <br /> K ; l .v ° <br /> H KH 0 <br />' z h a <br /> he 1 s <br /> UVB <br /> Figure 8. Notation in a vertical cross section. <br /> 9 <br />