Cooling Lake Simulations Compared to Thermal Imagery and Dye Tracers

We compare three-dimensional simulations of two cooling lakes at the Savannah River site to calibrated temperature data derived from high resolution thermal imagery and to data from two dye tracer experiments. The observed temperatures include detailed surface temperature maps created from calibrated thermal imagery and vertical temperature profiles measured at five locations across one of the cooling lakes. The dye tracer data consist of time series of concentrations recorded near the cooling water outlet of one of the cooling lakes. There is generally good agreement between observed and measured quantities, but the agreement is best for the smaller cooling lake that had a relatively higher heat load. We suggest that wind stress variability may have been at least partially responsible for the poorer agreement between observation and simulation for the larger cooling lake. The primary conclusion from this study is that thermal imagery is an excellent additional data source to dye tracer data for cooling lake model verification because imagery provides detailed information about the surface temperatures over the entire cooling lake allowing for a more complete verification of model simulations.

[1]  A. Garrett Drainage Flow Prediction with a One-Dimensional Model Including Canopy, Soil and Radiation Parameterizations. , 1983 .

[2]  H. L. Butler,et al.  Validation of Three‐Dimensional Hydrodynamic Model of Chesapeake Bay , 1993 .

[3]  C. Kranenburg,et al.  Quasi‐3D Numerical Modeling of Shallow‐Water Circulation , 1993 .

[4]  Tetsuji Yamada,et al.  Simulations of Nocturnal Drainage Flows by a q2l Turbulence Closure Model , 1983 .

[5]  A. Blumberg,et al.  Diagnostic and prognostic numerical circulation studies of the South Atlantic Bight , 1983 .

[6]  G. Mellor,et al.  Development of a turbulence closure model for geophysical fluid problems , 1982 .

[7]  B. Hicks Some evaluations of drag and bulk transfer coefficients over water bodies of different sizes , 1972 .

[8]  D. Harleman,et al.  Two-layer model for shallow horizontal convective circulation , 1980, Journal of Fluid Mechanics.

[9]  J. Louis A parametric model of vertical eddy fluxes in the atmosphere , 1979 .

[10]  K. I. Kondratʹev Radiation in the atmosphere , 1969 .

[11]  G. Jirka,et al.  Cooling Impoundments: Classification and Analysis , 1979 .

[12]  A. Garrett A comparison of the observed longwave radiation flux to calculations based on Kondratyev's and Brunt's methods , 1977 .

[13]  Alfred J. Garrett,et al.  A Parameter Study of Interactions Between Convective Clouds, the Convective Boundary Layer, and a Forested Surface , 1982 .

[14]  George L. Mellor,et al.  A Three-Dimensional Simulation of the Hudson Raritan Estuary. Part I: Description of the Model and Model Simulations , 1985 .

[15]  J. Smagorinsky,et al.  GENERAL CIRCULATION EXPERIMENTS WITH THE PRIMITIVE EQUATIONS , 1963 .

[16]  Ovid W. Eshbach,et al.  Eshbach's handbook of engineering fundamentals , 1952 .

[17]  A. Garrett Orographic cloud over the eastern slopes of Mauna Loa volcano, Hawaii, related to insolation and wind , 1980 .

[18]  K. Helfrich,et al.  Evaporation from heated water bodies: Predicting combined forced plus free convection , 1990 .