Local-in-time strong solvability of Navier--Stokes type variational inequalities by Rothe's method
Takahito Kashiwabara
TL;DR
This work develops a Rothe-time discretization framework to establish local-in-time strong solvability for Navier–Stokes type variational inequalities in a Hilbert space setting, without requiring the cancelation property $\langle B(u,v),v\rangle=0$ and under a stationarity-based regularity assumption on the Stokes problem. By combining a semi-implicit time scheme with a fully implicit monotone term $\varphi$, the authors derive uniform a priori estimates and prove existence and uniqueness of a local strong solution in the maximal-$L^2$ regularity class, and, under stronger data, in the Kiselev–Ladyzhenskaya class. A solvability theory for stationary and Oseen-type problems supports the time-discrete scheme, and the approach is illustrated through four concrete models: obstacle problems for convection–diffusion, nonlinear Neumann problems, Navier–Stokes with friction-type boundary conditions, and a Bingham flow with slip. The results extend the applicability of NS-type variational inequalities to broader boundary conditions and nonlinearities, providing a constructive, time-discretization-based pathway to local-in-time regular solutions in three dimensions. Overall, the paper advances a rigorous framework for local strong solvability of parabolic VIs with NS-type nonlinearities using Rothe’s method and stationary-stokes regularity assumptions.
Abstract
We consider parabolic variational inequalities in a Hilbert space $V$, which have a non-monotone nonlinearity of Navier--Stokes type represented by a bilinear operator $B: V \times V \to V'$ and a monotone type nonlinearity described by a convex, proper, and lower-semicontinuous functional $\varphi : V \to (-\infty, +\infty]$. Existence and uniqueness of a local-in-time strong solution in a maximal-$L^2$-regularity class and in a Kiselev--Ladyzhenskaya class are proved by discretization in time (also known as Rothe's method), provided that a corresponding stationary Stokes problem admits a regularity structure better than $V$ (which is typically $H^2$-regularity in case of the Navier--Stokes equations). Since we do not assume the cancelation property $\left< B(u, v), v \right> = 0$, in applications we may allow for broader boundary conditions than those treated by the existing literature.
