Global existence of strong solutions to a groundwater flow problem

preprint2020arXivOpen access

Abstract

In this paper we study the initial boundary value problem for the system $Δv= u_{x_1},\ u_t-\mbox{div}\left(\left((a|\mathbf{q}|+m)I+(b-a)\frac{\mathbf{q}\otimes\mathbf{q}}{|\mathbf{q}|}\right)\nabla u\right)=-\nabla u\cdot\mathbf{q}$, where q=(−vx2,vx1)T\mathbf{q}=(-v_{x_2}, v_{x_1})^T, q⊗q=qqT\mathbf{q}\otimes\mathbf{q}=\mathbf{q}\mathbf{q}^T. This problem has been proposed as a model for a fluid flowing through a porous medium under the influence of gravity and hydrodynamic dispersion. For each T>0T>0 we obtain a so-called strong solution (v,u)(v, u) in the function space L∞(0,T;(W1,∞(Ω))2)L^\infty(0,T; \left(W^{1,\infty}(Ω)\right)^2), where ΩΩ is a bounded domain in R2\mathbb{R}^2. The key ingredient in our approach is the decomposition $A^2=\mbox{tr} (A)A-\mbox{det}(A) I$ for any 2×22\times 2 symmetric matrix AA. By exploring this decomposition, we are able to derive an equation of parabolic type for the function (((a∣q∣+m)I+(b−a)q⊗q∣q∣)∇u⋅∇u)j,j≥1\left(\left((a|\mathbf{q}|+m)I+(b-a)\frac{\mathbf{q}\otimes\mathbf{q}}{|\mathbf{q}|}\right)\nabla u\cdot\nabla u\right)^j, j\geq 1. With the aid of this equation we obtain a uniform bound for ∇u\nabla u.

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