Inhomogeneous ows occuring naturally in the atmosphere and their in uence on the ow eld around wing pro les are examined. Inhomogeneous, in this context, means that at least one ow variable has a spatial gradient, and, in particular, a gradient in the velocity component normal to the velocity vector is considered. Well-known examples for such ows are shear winds, jet streams, low-level jet streams, the ow situation near the ground, and microbursts. Numerical simulations are performed for a NACA 0012 airfoil using a nite volume Euler code. They focus on two cases, namely, an idealized shear wind for parameter studies and a microburst. For the idealized shear wind, a linear velocity change is assumed. In the subsonic case, the additional velocities on the lower and upper side of the airfoil result in a positive additional lift and a negative pitching moment around the 25% axis. In the transonic regime, the effect on shock strength and shock position is dominant. For simulation of the ight through a microburst, a potential model for the velocity eld, consisting of a vortex ring parallel to the ground and a vortex ring of same strength mirrored at the ground, is applied. The chosen parameters simulate the Dallas-Fort Worth microburst. The analysis shows that the characteristics of the lift and moment coef cient follow that of the vertical velocity component, induced by the microburst. Rapid changes in the pitching moment with severe consequences on longitudinal stability occur. Nomenclature N A = Jacobian matrix for primitive variables (» direction) a = altitude c = speed of sound, coef cient c l , c m = lift coef cient, pitching moment coef cient c p = pressure coef cient e = total energy density, p=.· ¡ 1/ C ½.u 2 C v 2 /=2 F, G = uxes in curvilinear coordinates » andJ = determinant of the Jacobian of grid transformation l = length, airfoil chord M = Mach number M F = ight Mach number M l , M u = lower and upper Mach number in the idealized shear wind M y = vertical component of Mach number n = normal vector P k , P ¡1 k = matrix of the right and left eigenvectors of the nonconservativeEuler equations p = pressure Q = vector of conservative variables times J N Q = vector of primitive variables times J q = dynamic pressure t = time t = tangential vector u, v = velocity components in Cartesian coordinates x and y v = velocity vector W = vector of the characteristic variables x m = moment reference point x P , y P = position of the airfoil x 0 , x 1 = start and end position for the ight through the microburst Presented as Paper 99-3587 at the AIAA 30th Fluid y 0 , y 1 = lower and upper boundary of the idealized shear wind ® = angle of attack 1c p = difference in pressure coef cient, c p inhom ¡ c p hom 1M = change in incoming Mach number in the idealized shear wind 1M=1y = vertical gradient of Mach number in the idealized shear wind · = ratio of speci c heats K = diagonal matrix of the eigenvalues of N A » ,´= curvilinear coordinates ½ = density ¿ = transformed time due to coordinates » and¿ c = characteristic time 9 ...