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Diffusion of Lagrangian invariants in the Navier-Stokes equations

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Book cover Tubes, Sheets and Singularities in Fluid Dynamics

Part of the book series: Fluid Mechanics and Its Applications ((FMIA,volume 71))

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Abstract

The incompressible Euler equations can be written as the active vector system

$$ (\partial _t + u \cdot \nabla )A = 0$$

where u=W[A] is given by the Weber formula

$$ W[A] = P\{ (\nabla A)^* \upsilon \}$$

in terms of the gradient of A and the passive field v=u 0 (A). (P is the projector on the divergence-free part.) The initial data is A(x,0)=x, so for short times this is a distortion of the identity map. After a short time one obtains a new u and starts again from the identity map, using the new u instead of u 0 in the Weber formula. The viscous Navier-Stokes equations admit the same representation, with a diffusive back-to-labels map A and a v that is no longer passive.

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© 2002 Kluwer Academic Publishers

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Constantin, P. (2002). Diffusion of Lagrangian invariants in the Navier-Stokes equations. In: Bajer, K., Moffatt, H.K. (eds) Tubes, Sheets and Singularities in Fluid Dynamics. Fluid Mechanics and Its Applications, vol 71. Springer, Dordrecht. https://doi.org/10.1007/0-306-48420-X_35

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  • DOI: https://doi.org/10.1007/0-306-48420-X_35

  • Publisher Name: Springer, Dordrecht

  • Print ISBN: 978-1-4020-0980-8

  • Online ISBN: 978-0-306-48420-9

  • eBook Packages: Springer Book Archive

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