Recent atmospheric and wind tunnel data on the heat, mass and momentum transfer above natural and artificial surfaces indicate a general increase in the quantity kB −1 (= In(z o /z p ), where z p is the roughness length appropriate to the quantity p ) between aerodynamically smooth and fully rough flow. Below a roughness Reynolds number, u*z o /v , of about 100, kB −1 appears to be a single valued function of u*z o /v , closely approximated by the assumption of a molecular sub‐layer for heat and water vapour fluxes. Beyond u*z o /v = 100, there is no unique value of kB −1 , but rather the observations suggest that the behaviour falls into either of two categories. For surfaces comprised of arrays of widely spaced solid roughness elements, kB −1 continues to increase (with some evidence for a plateau being reached by about u*z o /v = 1,000, when kB −1 ≃ 10), whilst for surfaces comprised of randomly distributed fibrous roughness elements, kB −1 gradually decreases with increasing roughness Reynolds number beyond about 100.
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Garratt et al. (1973) studied this question.
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