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arxiv: 1106.3861 · v3 · pith:4ZXSM7AUnew · submitted 2011-06-20 · 🧮 math.AP · math.PR

Solution to the Navier-Stokes equations with random initial data

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keywords navier-stokesalphaequationssolutiondistributioninitialdatagamma
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We construct a solution to the spatially periodic $d$-dimensional Navier-Stokes equations with a given distribution of the initial data. The solution takes values in the Sobolev space $H^\alpha$, where the index $\alpha\in R$ is fixed arbitrary. The distribution of the initial value is a Gaussian measure on $H^\alpha$ whose parameters depend on $\alpha$. The Navier-Stokes solution is then a stochastic process verifying the Navier-Stokes equations almost surely. It is obtained as a limit in distribution of solutions to finite-dimensional ODEs which are Galerkin-type approximations for the Navier-Stokes equations. Moreover, the constructed Navier-Stokes solution $U(t,\omega)$ possesses the property: $$E[f(U(t,\omega))] = \int_{H^\alpha} f(e^{t\nu\Delta} u) \gamma(du)$$, where $f \in L_1(\gamma)$, $e^{t \Delta}$ is the heat semigroup, $\nu$ is the viscosity in the Navier-Stokes equations, and $\gamma$ is the distribution of the initial data.

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