Abstract
The Navier-Stokes equations appear as a singular perturbation of the Euler equations in which the small parameter ɛ is the viscosity or inverse of the Reynolds number. In many cases the convergence of the solutions of the Navier-Stokes equations to those of the Euler equations remains an outstanding open problem of mathematical physics. The result is not known in the case of the no-slip boundary condition, even in space dimension 2 for which the existence, uniqueness, and regularity of solution for all time is known for both the Navier-Stokes and Euler equations; see, e.g., [Kat84, Kat86, FT79, Tem75, Tem76, Tem01]. Fortunately, and this is the object of Chapters 6 and 7, this problem has been solved in a number of particular situations: special symmetries or boundary conditions other than the no-slip boundary condition.
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Notes
- 1.
The set \(\\mathcal{L}(H,\,D(A))\) denotes the space of bounded linear operators from H into D(A).
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Gie, GM., Hamouda, M., Jung, CY., Temam, R.M. (2018). The Navier-Stokes Equations in a Periodic Channel. In: Singular Perturbations and Boundary Layers. Applied Mathematical Sciences, vol 200. Springer, Cham. https://doi.org/10.1007/978-3-030-00638-9_6
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