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   <subfield code="a">ON THE NONLINEAR EVOLUTION OF INSTABILITY MODES IN UNSTEADY SHEAR LAYERS: THE STOKES LAYER AS A PARADIGM</subfield>
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   <subfield code="c">[XUESONG WU, STEPHEN J. COWLEY]</subfield>
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   <subfield code="a">The Stokes layer generated by a flat plate oscillating sinusoidally in an infinite fluid is an important prototype of unsteady flows. It is known to be susceptible to high-frequency instabilities at large Reynolds numbers. Linear theory shows that small disturbances can grow exponentially over part of a period, before becoming neutral at a later time. We show that at times when a disturbance is almost neutral, it can evolve through a weakly nonlinear stage. Our approach is a simple extension of previous non-equilibrium critical-layer theories developed for quasi-parallel flows. For any inviscidly unstable, unsteady shear layer, we present a unified explanation of the asymptotic scalings required to describe three distinct types of small disturbance. We then specialize to weakly nonlinear two-dimensional disturbances, and show that when the critical layer is ‘singular' the amplitude equation is of Hickernell's (1) integro-differential type. Solutions to this equation develop finitetime singularities if viscous effects are not too large. For the particular case of a Stokes layer, we find that for a class of disturbances with normalized wavenumbers in the range [0, 0-6] or [1-29, 1-43], the singularity can be eliminated by sufficiently large viscous effects; the instability wave then evolves to an equilibrium state. However, for wavenumbers in the range [0-6, 1-29], a finite-time singularity occurs no matter how large the scaled viscosity parameter is. This nonlinear explosive amplification may be related to the rapid growth of high-frequency disturbances observed as bursts in experiments.</subfield>
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