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The instability of an initially flat vortex sheet to a sinusoidal perturbation of the vorticity is studied by means of high-order Taylor series in time t . All finite-amplitude corrections are retained at each order in t . Our analysis indicates that the sheet develops a curvature singularity at t = t c < ∞. The variation of t c with the amplitude a of the perturbation vorticity is in good agreement with the asymptotic results of Moore. When a is O (1), the Fourier coefficient of order n decays slightly faster than predicted by Moore. Extensions of the present prototype of Kelvin-Helmholtz instability to other layered flows, such as Rayleigh-Taylor instability, are indicated.
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Meiron et al. (1982) studied this question.
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