How an airfoil generates lift is settled engineering practice—the Kutta–Joukovsky theorem relates lift to circulation, and the Kutta condition selects the observed flow—yet why the Kutta condition holds has again become a subject of discussion: since 2022 a variational theory of lift has proposed an inviscid selection principle based on Gauss’s principle of least constraint, prompting an ongoing debate in the archival literature. This review reassembles, in a self-contained way, the viscous answer given by matched asymptotic expansions. Three questions organise the presentation: what inviscid theory leaves undetermined and the logical status of the Kutta condition within it (Q1); whether boundary-layer theory and its higher-order completion, triple-deck theory, provide a deductive route from the Navier–Stokes equations to the Kutta condition together with quantitative predictions (Q2); and what this viscous route implies for the proposed inviscid selection principles (Q3). Starting from Blasius’ flat-plate solution and Goldstein’s near-wake, the triple-deck structure of the trailing-edge region is developed, and the resulting first-order corrections—the flat-plate drag correction and the lift-slope reduction cL/(2πα)=1−B with B=a1λ−5/4Re−3/8—are compared with wind-tunnel data, XFOIL and laminar Navier–Stokes solutions: the drag correction is confirmed quantitatively, the lift correction in sign, trend and order of magnitude over two decades of Reynolds number, and the domain of validity of the laminar theory is stated explicitly. The wake, with its transversely continuous pressure, enforces pressure continuity at the trailing edge and thereby fixes circulation and lift; any inviscid selection principle is constrained to reproduce this asymptotic limit. The viscous treatment of rounded trailing edges (Sychev–Smith separation combined with the Howarth–Sears wake condition) is outlined, and for bodies with smooth trailing edges a three-way quantitative test (variational vs. interactive boundary-layer/triple-deck vs. Navier–Stokes) is proposed, two legs of which already exist in the literature.
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Alois Peter Schaffarczyk (2026) studied this question.
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