Finite time singularities in a class of hydrodynamic models
Phys. Rev. E, 63, 056306 (2001) Models of inviscid incompressible fluid are considered, with the kinetic energy (i.e., the Lagrangian functional) taking the form ${\cal L}\sim\int k^\alpha|{\bf v_k}|^2d^3{\bf k}$ in 3D Fourier representation, where $\alpha$ is a constant, $0
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Zusammenfassung: | Phys. Rev. E, 63, 056306 (2001) Models of inviscid incompressible fluid are considered, with the kinetic
energy (i.e., the Lagrangian functional) taking the form ${\cal L}\sim\int
k^\alpha|{\bf v_k}|^2d^3{\bf k}$ in 3D Fourier representation, where $\alpha$
is a constant, $0 |
---|---|
DOI: | 10.48550/arxiv.physics/0012007 |