“…It is a well-known fact that the asymptotic Sherwood number for circular or parallel-plate duct with wall reaction (that is, with negligible washcoat diffusional limitations), varies from constant flux (Sh H,ϱ ) to constant concentration (Sh T,ϱ ) asymptote as s 2 varies from 0 to ϱ (Gupta and Balakotaiah, 2001;Tronconi and Forzatti, 1992). For these geometries, the constant flux asymptotes of first (Sh H 1 ,ϱ ) and second (Sh H 2 ,ϱ ) kind are the same because of the 1-D diffusion in the transverse direction, whereas they differ from each other for channels with other geometries, such as square, triangle, and so forth, where transverse diffusion is 2-D. Table 1 lists the values for the asymptotic Sherwood or Nusselt numbers for some commonly used channel geometries.…”