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In order to account for entrance effects, the flow channel length averaged Sherwood number can be expressed as a function of the Graetz number for mass transfer in a circular tube with a correlation similar to that for heat transfer. Simonson and Besant (1997) showed that the entrance effects in the flow channels of an energy wheel are usually small and will be negligible when the Graetz number for the flow channel length is large. The only dimensionless number for this problem is the Graetz number U[H. |
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