Resonance phenomenon for the Galerkin-truncated Burgers and Euler equations
arXiv:1011.1826 · doi:10.1103/PhysRevE.84.016301
Abstract
It is shown that the solutions of inviscid hydrodynamical equations with suppression of all spatial Fourier modes having wavenumbers in excess of a threshold exhibit unexpected features. The study is carried out for both the one-dimensional Burgers equation and the two-dimensional incompressible Euler equation. For large and smooth initial conditions, the first symptom of truncation, a localized short-wavelength oscillation which we call a "tyger", is caused by a resonant interaction between fluid particle motion and truncation waves generated by small-scale features (shocks, layers with strong vorticity gradients, etc). Tygers appear when complex-space singularities come within one Galerkin wavelength $\lambdag = 2π/K_G$ from the real domain and arise far away from preexisting small-scale structures at locations whose velocities match that of such structures. Tygers are weak and strongly localized at first - in the Burgers case at the time of appearance of the first shock their amplitudes and widths are proportional to and respectively - but grow and eventually invade the whole flow. They are thus the first manifestations of the thermalization predicted by T.D. Lee in 1952. The sudden dissipative anomaly - the presence of a finite dissipation in the limit of vanishing viscosity after a finite time -, which is well known for the Burgers equation and sometimes conjectured for the 3D Euler equation, has as counterpart, in the truncated case, the ability of tygers to store a finite amount of energy in the limit . This leads to Reynolds stresses acting on scales larger than the Galerkin wavelength and prevents the flow from converging to the inviscid-limit solution. There are indications that it may eventually be possible to purge the tygers and thereby to recover the correct inviscid-limit behavior.
23 pages, 21 figures
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