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PNNL-13501 - Pacific Northwest National Laboratory

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shown in Figure 1. Simulated results matched observed<br />

data well: observed drop angle = 57-deg, simulated = 55deg;<br />

observed downstream/drop depth = 0.094, simulated<br />

downstream/drop depth = 0.088, observed brink/drop<br />

depth=0.18, simulated brink/drop depth = 0.15.<br />

Figure 1. Evolution through time of the numerical model’s<br />

solution for a drop structure. Contours relate to velocity<br />

magnitude.<br />

A second, commercially available three-dimensional<br />

hydrodynamic model, STAR-CD, was used to simulate<br />

the larger scale flow field upstream and downstream of<br />

the Bonneville Project. These flows were simulated in a<br />

steady-state mode using a rigid lid approximation (nonfree<br />

surface). These two assumptions simplify the<br />

numerical complexity, allowing for greater grid mesh<br />

detail. STAR-CD was applied to the forebay, intakes, and<br />

tailwater of the Bonneville Dam Project.<br />

The model was verified by simulating February 7, 2000,<br />

field conditions. Inflow boundary conditions for the First<br />

and Second Powerhouses and Spillway were set using<br />

recorded Project operations. Bottom roughness was<br />

estimated using a Manning’s n value of 0.020. Results<br />

showing simulated water velocities downstream of the<br />

Bonneville Project are shown in Figure 2.<br />

Figure 2. Numerically generated contours of velocity<br />

magnitude downstream of the Bonneville Project<br />

128 FY 2000 <strong>Laboratory</strong> Directed Research and Development Annual Report<br />

Model data was then compared to water velocity data<br />

collected using an acoustic Doppler current profiler.<br />

Water velocities were compared at three depths through<br />

the water column. A graphical comparison of observed<br />

versus modeled data is shown in Figure 3.<br />

Figure 3. Close-up of velocity magnitude contours near the<br />

second powerhouse. Arrows compare numerical and<br />

observed data at various locations.<br />

Simulating Fish Behavior<br />

Steady-state hydrodynamic results from the STAR-CD<br />

application to the Bonneville tailrace were used as input<br />

to NWGrid, developed by Harold Trease of <strong>PNNL</strong>.<br />

NWGrid is capable of simulating the evolution of<br />

particles introduced into the flow field. In addition, these<br />

particles can be assigned various statistical properties<br />

representing fish behavior. This ongoing area of research<br />

is only beginning hence behavioral properties were<br />

appropriately simplistic for this project. For the purposes<br />

of this project, the “fish” particles were given a simple<br />

uniform normal random distribution (Figure 4).<br />

Figure 4. “Fish” particles entering Unit 5 of the first<br />

powerhouse. Foreground structure is a prototype surface<br />

collector which isolates flow from two of the turbine bays.

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