Mean velocity profiles of Couette·Poiseuille-type turbulent flow developed between fixed and moving walls have been measured. The relevant parameters for the wall, 1/2-power and core region are μ(=μ
3*/αν, where α=1/ρ·dτ/dy) and Re
*'(=u
*h'/ν), β'(=αh'/u
2*) and Re
*', and β(=αh/u
2*) and Re
* (=u
*h/ν) respectively. The effects of these parameters on the velocity profiles in each region considered. Except for the core region of the Couette-type flow, each region has a reference wall. In the wall region, the wall law varies largely with μ but slightly with Re
*'. Typically, the additive constant B of the logarithmic-velocity low (or Van-Driest damping factor A
+) is shown to depend only on μ. The 1/2-power velocity law depends not only on β', as well known, but also Re
*' under low Re conditions. In the core region, the normalized eddy viscosity ε
T/u
*h' is constant irrespective of Re
* and β for Poiseuille-type flow while it depends on both Re
* and β for Couette-type flow. This indicates that the turbulent structures of the core region are quite different between Poiseuille-and Couette-type flows.
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