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Seaside Model Report<br />

October 26, 2007<br />

Model Development<br />

of the <strong>model</strong> domain also is a no-<strong>flow</strong> boundary. Likewise, the boundary conditions on<br />

the l<strong>and</strong>ward <strong>and</strong> seaward vertical surfaces of the <strong>model</strong> domain, except for the segment<br />

of the Reliz Fault described above, are no-<strong>flow</strong> boundaries.<br />

The leakances for the specified-head boundaries were assigned so as to produce a<br />

computed head almost identical to the specified head. Accordingly, the leakances were<br />

set to a somewhat arbitrary large value. The leakances were set sufficiently large to<br />

produce nearly identical specified <strong>and</strong> computed heads, but they were set also such that<br />

the difference between the specified <strong>and</strong> computed heads was with the precision of the<br />

computer.<br />

Solute Transport<br />

Where water crosses boundary surfaces as inward <strong>flow</strong>s, due either to the<br />

assignment of specified-head or non-zero specified-flux <strong>groundwater</strong>-<strong>flow</strong> boundaries,<br />

the salinity of the inward <strong>flow</strong> is assigned. However, except for the boundary surface<br />

representing the bottom of Monterey Bay, the specified salinity equals zero. For the<br />

Monterey Bay surface, the specified salinity equals unity, which is the dimensionless<br />

concentration equivalent to seawater.<br />

3.1.6 Initial Conditions<br />

The <strong>groundwater</strong>-<strong>flow</strong> <strong>and</strong> solute-<strong>transport</strong> initial conditions is an assumed<br />

steady-state condition at the end of 1955. The <strong>groundwater</strong> development at the time was<br />

minimal at that time relative to precipitation recharge, <strong>and</strong> initial conditions were<br />

simulated based on the assumed steady state.<br />

Groundwater Flow<br />

The initial heads for <strong>groundwater</strong> <strong>flow</strong> are the calculated steady-state heads<br />

representing the long-term average annual recharge, the 1956 <strong>groundwater</strong> pumping, <strong>and</strong><br />

the boundary conditions described above. FEMFLOW3D can calculate steady-state initial<br />

heads within a transient-state simulation, <strong>and</strong> that facility was used to specify the initial<br />

heads for the Seaside <strong>groundwater</strong> <strong>basin</strong>. The resulting steady-state <strong>groundwater</strong> levels<br />

are shown on Figures 3.10a-b. Because the steady-state heads depend on the hydraulic<br />

parameters assigned to the hydrogeologic units represented in the <strong>model</strong>, Figures 3.10a-b<br />

are derived from the <strong>model</strong> calibration, which is described later.<br />

Solute Transport<br />

The initial salinity for solute <strong>transport</strong> are the calculated nearly steady-state<br />

salinity again representing the long-term average annual recharge, the 1956 <strong>groundwater</strong><br />

pumping, <strong>and</strong> the boundary conditions described above. By this construction of initial<br />

conditions, the seawater intrusion in the seaward part of the Seaside <strong>basin</strong> is assumed to<br />

be in equilibrium with the 1956 steady-state <strong>groundwater</strong> <strong>flow</strong>. Calculating steady-state<br />

solute-<strong>transport</strong> with FEMFLOW3D is not as convenient as for calculating steady-state<br />

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