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Near and Far Field Dilution Analysis of Manteca Discharge October 2006 <br /> using two discharge cases: the first with the current side bank discharge, and the second, <br /> a preliminary design diffuser. Both cases were run for different river flow conditions and <br /> with different discharge rates to simulate SIP critical conditions (SWRCB, 2005). <br /> Model Description <br /> The finite element representation of the San Joaquin River used for the Manteca near <br /> field dilution modeling extends from the gage at Vernalis to the bifurcation at the head of <br /> Old River as shown in Figure 1. The model includes one-dimensional cross-sectionally <br /> averaged sections at the upstream and down stream ends and a two-dimensional depth- <br /> averaged section extending from below Mossdale Bridge to just upstream of the outfall. <br /> Details of the entire 2-D section of the finite element mesh are shown in Figure 2, and the <br /> immediate vicinity of the outfall is shown in Figure 3 and Figure 4 with the side bank <br /> discharge and with the diffuser, respectively. Three-D views of the network, colored by <br /> depth, are shown in Figure 5 and Figure 6 with the side bank discharge and the diffuser, <br /> respectively,where the lines show the projection of the individual element on the channel <br /> bottom and the shaded areas show the shape and location of cross sections that are <br /> referenced below. The bridge piers appear as holes in the networks. <br /> For the side bank discharge simulations, effluent is input to the first two elements of the <br /> side bank discharge channel, as shown in Figure 7. For the diffuser simulations, effluent <br /> is input to the 16 elements making up the diffuser(Figure 8). The diffuser is 140 feet <br /> long, located in the deepest section of the channel on the eastern side of the San Joaquin <br /> River, extending out from the location of the existing side bank discharge. Diffuser <br /> elevations follow the existing channel contours. <br /> 2 <br />