Instability of Unidirectional Flows for the 2D Navier–Stokes Equations and Related $$\alpha $$-Models
Autor: | Shibi Vasudevan |
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Rok vydání: | 2021 |
Předmět: |
Physics
Direct sum Applied Mathematics Operator (physics) 010102 general mathematics Fredholm determinant Condensed Matter Physics 01 natural sciences Method of continued fractions Physics::Fluid Dynamics 010101 applied mathematics Computational Mathematics Cover (topology) 0101 mathematics Trace class Fourier series Mathematical Physics Eigenvalues and eigenvectors Mathematical physics |
Zdroj: | Journal of Mathematical Fluid Mechanics. 23 |
ISSN: | 1422-6952 1422-6928 |
DOI: | 10.1007/s00021-021-00568-0 |
Popis: | We study instability of unidirectional flows for the linearized 2D Navier–Stokes equations on the torus. Unidirectional flows are steady states whose vorticity is given by Fourier modes corresponding to a single vector $${\mathbf {p}} \in {\mathbb {Z}}^{2}$$ . Using Fourier series and a geometric decomposition allows us to decompose the linearized operator $$L_{B}$$ acting on the space $$\ell ^{2}({\mathbb {Z}}^{2})$$ about this steady state as a direct sum of linear operators $$L_{B,{\mathbf {q}}}$$ acting on $$\ell ^{2}({\mathbb {Z}})$$ parametrized by some vectors $${\mathbf {q}}\in {\mathbb {Z}}^2$$ . Using the method of continued fractions we prove that the linearized operator $$L_{B,{\mathbf {q}}}$$ about this steady state has an eigenvalue with positive real part thereby implying exponential instability of the linearized equations about this steady state. We further obtain a characterization of unstable eigenvalues of $$L_{B,{\mathbf {q}}}$$ in terms of the zeros of a perturbation determinant (Fredholm determinant) associated with a trace class operator $$K_{\lambda }$$ . We also extend our main instability result to cover regularized variants (involving a parameter $$\alpha >0$$ ) of the Navier–Stokes equations, namely the second grade fluid model, the Navier–Stokes- $$\alpha $$ and the Navier–Stokes–Voigt models. |
Databáze: | OpenAIRE |
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