Smooth 2D Euler steady states with multiple critical points can be perturbed to make vorticity non-functional in the stream function, yielding isolated branches of stable states unlike the analytic case.
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Vanishing viscosity selects constant-vorticity flows in bounded domains and shear flows in strips as the only possible limits for 2D steady Euler equations.
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On the flexibility of 2D Euler steady states
Smooth 2D Euler steady states with multiple critical points can be perturbed to make vorticity non-functional in the stream function, yielding isolated branches of stable states unlike the analytic case.
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A selection principle for 2D steady Euler flows via the vanishing viscosity limit
Vanishing viscosity selects constant-vorticity flows in bounded domains and shear flows in strips as the only possible limits for 2D steady Euler equations.