“…Along the free boundaries, where the flow field is considered fully developed, the gradients normal to the boundary and normal velocity vanish as: (Equation 10) At the outlet computation domain, which placed at x/H = 25.5 downstream of the cylinder, a zero streamwise gradient is specified as: (Equation 11) In the near‐porous wall region, which has two sub‐layers, two different formulas have been used in computational algorithm. Regarding y‐direction as normal direction, the viscous sub‐layer was simulated as (Equation 12) and in the log‐law layer (Equation 13) has been regarded with the constants of u p + = y p + = 11.5 and κ = 0.4 (Çuhadaroğlu, 2004). Finally, the WFs used in this study can be summarized as follows: (Equation 14) Near the wall, the log‐law region is in local equilibrium so that the rate of turbulence kinetic energy production is approximately equal to its dissipation rate.…”