“…Since it is assumed that 2s c, and that changes in the flow happen on the span length-scale, the problem can be considered as 2D. The problem consists of a symmetric airfoil at a certain spanwise section undergoing small-amplitude pitch and plunge oscillations, h(y, t) = h * 0 (y)c(y)e iωt α(y, t) = α 0 (y)e i(ωt+ψ) (7) where h * 0 is plunge amplitude per unit chord, α 0 is pitch amplitude, ψ is the phase between plunge and pitch, and ω is the frequency of oscillation typically expressed as a chordwise or spanwise reduced frequency Figure 2 shows this problem, for which the solution is given by Theodorsen [60]. The results are expressed here in terms of a general unsteady thin-airfoil theory [36,52] which allows easy modification of the approach for various wing geometries and kinematics.…”