“…The other is the scheme from Choi and Hong (, hereafter C15), which considers the effects of GWD together with LLWD (Hong et al, ; Kim & Arakawa, ) and FBD (Kim & Doyle, ) with improved parameters (e.g., height of the blocked layer). The wave stress due to both of the GWD and LLWD at reference level ( τ W ) is given as follows: where E is the enhancement factor for representing the nonlinear enhancement of drag due to the low‐level wave breaking, which is calculated by the orographic asymmetry (OA), which represents the shape and location of subgrid‐scale orography relative to the grid, and the Froude number Fr 0 (= h OD N 0 / U 0 ) normalized by its critical value ( Fr c = 1); OD is the orographic direction, which is equivalent to the horizontal aspect ratio of the orography; m is the number of subgrid‐scale orography and L x represents the subgrid‐scale mountain width in the direction of low‐level wind; λ eff is the effective grid length; G is an asymptotic function that provides a smooth transition between the nonblocking and blocking cases and includes the effect of orographic convexity (OC) corresponding to the vertical orographic aspect ratio; and C E and C G are set to 0.8 and 0.5, respectively, based on the mesoscale simulation results from Kim and Arakawa ().…”