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Existence and uniqueness of weak solutions for the generalized stochastic Navier-Stokes-Voigt equations

Ankit Kumar, Hermenegildo Borges de Oliveira, Manil T. Mohan

Abstract

In this work, we consider the incompressible generalized Navier-Stokes-Voigt equations in a bounded domain $\mathcal{O}\subset\mathbb{R}^d$, $d\geq 2$, driven by a multiplicative Gaussian noise. The considered momentum equation is given by: \begin{align*} \mathrm{d}\left(\boldsymbol{u} - κΔ\boldsymbol{u}\right) = \left[\boldsymbol{f} +\operatorname{div} \left(-π\mathbf{I}+ν|\mathbf{D}(\boldsymbol{u})|^{p-2}\mathbf{D}(\boldsymbol{u})-\boldsymbol{u}\otimes \boldsymbol{u}\right)\right]\mathrm{d} t + Φ(\boldsymbol{u})\mathrm{d} \mathrm{W}(t). \end{align*} In the case of $d=2,3$, $\boldsymbol{u}$ accounts for the velocity field, $π$ is the pressure, $\boldsymbol{f}$ is a body force and the final term stay for the stochastic forces. Here, $κ$ and $ν$ are given positive constants that account for the kinematic viscosity and relaxation time, and the power-law index $p$ is another constant (assumed $p>1$) that characterizes the flow. We use the usual notation $\mathbf{I}$ for the unit tensor and $\mathbf{D}(\boldsymbol{u}):=\frac{1}{2}\left(\nabla \boldsymbol{u} + (\nabla \boldsymbol{u})^{\top}\right)$ for the symmetric part of velocity gradient. For $p\in\big(\frac{2d}{d+2},\infty\big)$, we first prove the existence of a martingale solution. Then we show the pathwise uniqueness of solutions. We employ the classical Yamada-Watanabe theorem to ensure the existence of a unique probabilistic strong solution.Then we show the pathwise uniqueness of solutions. We employ the classical Yamada-Watanabe theorem to ensure the existence of a unique probabilistic strong solution.

Existence and uniqueness of weak solutions for the generalized stochastic Navier-Stokes-Voigt equations

Abstract

In this work, we consider the incompressible generalized Navier-Stokes-Voigt equations in a bounded domain , , driven by a multiplicative Gaussian noise. The considered momentum equation is given by: \begin{align*} \mathrm{d}\left(\boldsymbol{u} - κΔ\boldsymbol{u}\right) = \left[\boldsymbol{f} +\operatorname{div} \left(-π\mathbf{I}+ν|\mathbf{D}(\boldsymbol{u})|^{p-2}\mathbf{D}(\boldsymbol{u})-\boldsymbol{u}\otimes \boldsymbol{u}\right)\right]\mathrm{d} t + Φ(\boldsymbol{u})\mathrm{d} \mathrm{W}(t). \end{align*} In the case of , accounts for the velocity field, is the pressure, is a body force and the final term stay for the stochastic forces. Here, and are given positive constants that account for the kinematic viscosity and relaxation time, and the power-law index is another constant (assumed ) that characterizes the flow. We use the usual notation for the unit tensor and for the symmetric part of velocity gradient. For , we first prove the existence of a martingale solution. Then we show the pathwise uniqueness of solutions. We employ the classical Yamada-Watanabe theorem to ensure the existence of a unique probabilistic strong solution.Then we show the pathwise uniqueness of solutions. We employ the classical Yamada-Watanabe theorem to ensure the existence of a unique probabilistic strong solution.
Paper Structure (20 sections, 13 theorems, 243 equations)

This paper contains 20 sections, 13 theorems, 243 equations.

Key Result

Lemma 2.1

Let the map $\mathbf{M}:[0,T]\times\mathbb{R}^d\times\Omega\longrightarrow\mathcal{M}^{d\times d}(\mathbb{R})$, defined by $(t, x, \omega)\mapsto \mathbf{M}=\mathbf{M}(t, x, \omega)$, and $\mathbf{b}:[0,T]\times\mathbb{R}^d\times\Omega\longrightarrow\mathbb{R}^d$, defined by $(t, x, \omega)\mapsto \ where $K_t(R)$ is an $\mathbb{R}^+-$valued process adapted to the filtration $\{\mathscr{F}_t\}_{t\

Theorems & Definitions (41)

  • Lemma 2.1
  • proof
  • Lemma 2.2
  • proof
  • Definition 2.3
  • Definition 2.4: Probabilistically strong solution
  • Definition 2.5: Pathwise uniqueness
  • Theorem 2.6
  • Theorem 2.7
  • Theorem 3.1
  • ...and 31 more