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which correlates well with the data as shown in Figure 6. Note also that Equation (25) reduces to (21) as . For Re=0.1, the predictions of Equations (20) and (21) are shown in Figure 6 for comparison. It is seen that the prediction of Equation (20) for the diffusion limit is in good agreement with the result of (25) for small Peclet numbers. Similarly the prediction of Equation (21) for the interception limit asymptotes the empirical Equation (25) at large Peclet numbers.
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Dr. Goodarz Ahmadi |
Turbulence & Multiphase Fluid Flow Laboratory |
Department of Mechanical & Aeronautical Engineering
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