Abstract

The bifurcation of steady waves from (irrotational) inviscid streamflows is considered. The flux Q is scaled to unity to leave two quantities R (pressure head) and S (flowforce) parametrizinig the wavetrain. In a well-known paper, Bcnjamin and Lighthill (Proc. R. Soc. A 224 (1954) 448-460) presented calculations within a novel version of cnoidal wave theory which suggested that the coordinate pairs of R and S lie inside the cusped locus traced by the sub- and supercritical streamflows, and conjectured that this was the case for all irrotational water waves. Recently, the author described explicitly how wave branches, representing (Stokes') periodic waves bifurcating from the streamflow branch, point locally inside the streamflow cusp in the (R, S) diagram. In addition, accurate numerics showed how these constant-period branches extend globally towards the wave of greatest height.

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