========================================================================================================= Wall-resolved LES database of A-Airfoil near stall condition at 13.3 deg, Re_c = 2.1E6, M = 0.15 Originally uploaded on December 20, 2019 Updated on September 24, 2020 Copyright (c) Soshi Kawai. All Rights Reserved. Contact: kawai@tohoku.ac.jp ========================================================================================================= Original paper: Kengo Asada & Soshi Kawai, "Large-eddy simulation of airfoil flow near stall condition at Reynolds number 2.1 \times 10^6," Physics of Fluids, 30 (8), 085103, (2018). Related paper (Wall-modeled LES at the same condition): Yoshiharu Tamaki, Yuma Fukushima, Yuichi Kuya & Soshi Kawai, "Physics and modeling of trailing-edge stall phenomena for wall-modeled large-eddy simulation" Physical Review Fluids (5), 074602, 2020. (Note: minus of - in Fig 10 (b) is missing) ========================================================================================================= This database is for the grid CM3 in the paper and includes # surface data.txt x/c C_p C_f H (shape factor) Re_theta (Re based on the momentum thickness) Re_delta_star (Re based on the displacement thickness) # profiles_{x/c coordinate}.txt Y/c (wall normal coordinate) (mean wall-parallel velocity, normalized by freestrem velocity) (Reynolds normal stress in the streamwise direction, normalized by u_inf^2) (Reynolds normal stress in the wall-normal direction, normalized by u_inf^2) (Reynolds normal stress in the spanwise direction, normalized by u_inf^2) - (Reynolds shear stress, normalized by u_tau^2) y+ U+= /u_tau (Reynolds normal stress in the streamwise direction, normalized by u_tau^2) (Reynolds normal stress in the wall-normal direction, normalized by u_tau^2) (Reynolds normal stress in the spanwise direction, normalized by u_tau^2) - (Reynolds shear stress, normalized by u_tau^2) # budget_{x/c coordinate}.txt (momentum budget, see Fig. 20 of the original paper) Y/c convection (normalized by u_inf^2/c) viscous (normalized by u_inf^2/c) pressure_gradient (normalized by u_inf^2/c) Reynolds_stress (normalized by u_inf^2/c) # 2D data (C binary, little-endian, single precision, near-field cropped) - grid_2d.xyz # (imax, jmax) = 4941 x 288 read(iu) imax,jmax read(iu) ((x(i,j),i=1,imax),j=1,jmax),((y(i,j),i=1,imax),j=1,jmax) - statistics_2d.fun # (imax, jmax) = 4941 x 288 # (nvar) = 8 read(iu) imax,jmax,nvar read(iu) (((data(i,j,n),i=1,imax),j=1,jmax),n=1,nvar) data(i,j,1): Mean density, rho/rho_inf data(i,j,2): Mean x-velocity, u/u_inf data(i,j,3): Mean y-velocity, v/u_inf data(i,j,4): Mean pressure, p/p_inf data(i,j,5): Reynolds normal stress in x direction, (u'u')/(u_inf^2) data(i,j,6): Reynolds normal stress in y direction, (v'v')/(u_inf^2) data(i,j,7): Reynolds normal stress in z direction, (w'w')/(u_inf^2) data(i,j,8): Reynolds shear stress, (-u'v')/(u_inf^2) (u, v, w) are the velocities in the Cartesian coordinates (x, y, z) (w being the spanwise velocity) =========================================================================================================