Navier-Stokes Mini Application

The solver implemented in this miniapp solves the transient incompressible Navier-Stokes equations.

Theory

The equations are given in the non-dimensionalized form

\begin{align} \frac{\partial u}{\partial t} + (u \cdot \nabla) u - \frac{1}{Re} \nabla^2 u + \nabla p &= f & \quad \text{in } \Omega\\ \nabla \cdot u &= 0 & \quad \text{in } \Omega \end{align}

where $Re$ represents the Reynolds number. In order to solve these equations, the method presented in Tomboulides (1997)1 is used, which is based on an equal order finite element discretization on quadrilateral or hexahedral elements of high polynomial order. The method describes an implicit-explicit time-integration scheme for the viscous and convective terms respectively. Introducing the following notation the nonlinear term $N(u) = -(u \cdot \nabla) u$ and the time-extrapolated form

\begin{align} \label{eq:Next} N^*(u^{n+1}) = \sum_{j=1}^k a_j N(u^{n+1-j}) \end{align}

where $a_j$ are coefficients from the corresponding explicit time integration method.

Applying a BDF method with coefficients $b_j$ to the initial equation using the introduced forms yields

\begin{align} \sum_{j=0}^k \frac{b_j}{\Delta t} u^{n+1-j} = -\nabla p^{n+1} + L(u^{n+1}) + N^*(u^{n+1}) + f^{n+1}. \end{align}

Collecting all known quantities at a given time with

\begin{align} F^*(u^n) = -\sum_{j=1}^k \frac{b_j}{\Delta t} u^{n+1-j} + N^*(u^{n+1}) + f^{n+1} \end{align}

the BDF expression reduces to

\begin{align} \label{eq:bdf_short} \frac{b_0}{\Delta t} u^{n+1} = -\nabla p^{n+1} + L(u^{n+1}) + F^*(u^n). \end{align}

To achieve a high order convergence in space the linear term $L(u)$ is replaced by

\begin{align} L_{\times}(u) = \nu \nabla(\nabla \cdot u) - \nu \nabla \times \nabla \times u \end{align}

which is used to weakly enforce incompressibility by setting the first term to zero. Like in \eqref{eq:Next} we introduce the time extrapolated term

\begin{align} L^*_{\times}(u) = \sum_{j=1}^k a_j L_{\times}(u^{n+1-j}). \end{align}

To compute the pressure we rearrange \eqref{eq:bdf_short} and take the divergence on both sides

\begin{align} \label{eq:prespois} \nabla^2 p^{n+1} = \nabla \cdot (L_{\times}^*(u^{n+1} + F^*(u^{n+1})), \end{align}

which is closed by the Neumann type boundary condition

\begin{align} \nabla p^{n+1} \cdot \hat{n} = -\frac{b_0}{\Delta t} u^{n+1} \cdot \hat{n} + (L_{\times}^*(u^{n+1} + F^*(u^{n+1})) \cdot \hat{n}. \end{align}

We will refer to this as the pressure Poisson equation in the following. The last step is a Helmholtz type equation to solve for the implicit (viscous) velocity part which is also derived from \eqref{eq:bdf_short}. Consider

\begin{align} \label{eq:hlm} \frac{b_0}{\Delta t} u^{n+1} - L(u^{n+1}) = -\nabla p^{n+1} + F^*(u^{n+1}) \end{align}

with the Dirichlet (essential type) boundary condition

\begin{align} u^{n+1} = g_D^{n+1}. \end{align}

A detailed walk through can also be found in Franco et al (2020) 2.

Note The notation is very similar to what is used in the code to make it easy to follow the theoretical explanation and understand what is done in the implementation.

Boundary Conditions

Inflow and no-slip walls

For inflow or no-slip wall boundary conditions one should use the method NavierSolver::AddVelDirichletBC. This enforces the value on $u^{n+1}$ in \eqref{eq:hlm}. It is valid to call this method multiple times on different boundary attributes of the mesh. The NavierSolver instance keeps track of the associated Coefficient and accompanying boundary attribute. The passed attribute array can be modified, deleted or reused, since a copy is created.

Pressure outlet

If an outlet of a domain is supposed to represent a pressure outlet (e.g. zero-pressure), one should use the method NavierSolver::AddPresDirichletBC. This enforces the pressure value $p^{n+1}$ in \eqref{eq:prespois}.

Zero-stress

This boundary condition is used to represent an outflow attribute. Due to the nature of the $H^1$ finite-element discretization, the terms arise naturally in \eqref{eq:prespois} and \eqref{eq:hlm} resulting in

\begin{align} \nu \nabla u \cdot \hat{n} - p \mathbb{I} \cdot \hat{n} = 0, \end{align}

where $\mathbb{I}$ represents the identity tensor.

If there is no other boundary condition applied to a certain attribute, this boundary condition is applied automatically (not through modification but rather through the formulation).

Solvers and preconditioners

The choice of solvers and preconditioners for \eqref{eq:prespois} and \eqref{eq:hlm} are essential for the performance and robustness of the simulation.

The pressure Poisson equation \eqref{eq:prespois} is solved using the CG Krylov method in combination with the low-order refined preconditioning technique coupled with AMG (c.f. Franco et al (2020)2).

Due to the nature of the explicit time discretization of the nonlinear term, the method used is CFL (and therefore time step) bound. As a result the time derivative term in \eqref{eq:hlm} is dominating and a CG Krylov method preconditioned with Jacobi is sufficient.

Depending on the problem, this results in the majority of time per time step being spent in the pressure Poisson solve.

At the moment there is no interface to change the default options for the solvers, but a user can easily modify them in the code itself.

FAQ


  1. A. G. Tomboulides, J. C. Y. Lee & S. A. Orszag (1997) Numerical Simulation of Low Mach Number Reactive Flows 

  2. Michael Franco, Jean-Sylvain Camier, Julian Andrej, Will Pazner (2020) High-order matrix-free incompressible flow solvers with GPU acceleration and low-order refined preconditioners (https://arxiv.org/abs/1910.03032)