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Figure 12.2 Time histories of 1-m temperature, friction velocity u
, and surface
temperature flux Q 0 measured in the 1973 Minnesota experiment. From Caughey
et al . ( 1979 ).
Figure 12.3 The late-afternoon decay of the friction velocity u
in Run 2 of the
1973 Minnesota experiment. The solid line is the prediction of a second-order-
closure model. From Wyngaard ( 1975 ).
mean rate of energy loss through viscous dissipation is balanced by their mean
rate of gain through the Kolmogorov energy cascade (Chapter 6) . If the rate of
viscous dissipation were larger than the cascade rate, the kinetic energy of the
dissipative eddies would decrease, decreasing the dissipation rate - and vice versa.
 
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