# Compressible Navier-Stokes mini-app¶

This example is located in the subdirectory examples/fluids. It solves the time-dependent Navier-Stokes equations of compressible gas dynamics in a static Eulerian three-dimensional frame using unstructured high-order finite/spectral element spatial discretizations and explicit or implicit high-order time-stepping (available in PETSc). Moreover, the Navier-Stokes example has been developed using PETSc, so that the pointwise physics (defined at quadrature points) is separated from the parallelization and meshing concerns.

The mathematical formulation (from [GRL10], cf. SE3) is given in what follows. The compressible Navier-Stokes equations in conservative form are

(15)\begin{aligned} \frac{\partial \rho}{\partial t} + \nabla \cdot \bm{U} &= 0 \\ \frac{\partial \bm{U}}{\partial t} + \nabla \cdot \left( \frac{\bm{U} \otimes \bm{U}}{\rho} + P \bm{I}_3 -\bm\sigma \right) + \rho g \bm{\hat k} &= 0 \\ \frac{\partial E}{\partial t} + \nabla \cdot \left( \frac{(E + P)\bm{U}}{\rho} -\bm{u} \cdot \bm{\sigma} - k \nabla T \right) &= 0 \, , \\ \end{aligned}

where $$\bm{\sigma} = \mu(\nabla \bm{u} + (\nabla \bm{u})^T + \lambda (\nabla \cdot \bm{u})\bm{I}_3)$$ is the Cauchy (symmetric) stress tensor, with $$\mu$$ the dynamic viscosity coefficient, and $$\lambda = - 2/3$$ the Stokes hypothesis constant. In equations (15), $$\rho$$ represents the volume mass density, $$U$$ the momentum density (defined as $$\bm{U}=\rho \bm{u}$$, where $$\bm{u}$$ is the vector velocity field), $$E$$ the total energy density (defined as $$E = \rho e$$, where $$e$$ is the total energy), $$\bm{I}_3$$ represents the $$3 \times 3$$ identity matrix, $$g$$ the gravitational acceleration constant, $$\bm{\hat{k}}$$ the unit vector in the $$z$$ direction, $$k$$ the thermal conductivity constant, $$T$$ represents the temperature, and $$P$$ the pressure, given by the following equation of state

(16)$P = \left( {c_p}/{c_v} -1\right) \left( E - {\bm{U}\cdot\bm{U}}/{(2 \rho)} - \rho g z \right) \, ,$

where $$c_p$$ is the specific heat at constant pressure and $$c_v$$ is the specific heat at constant volume (that define $$\gamma = c_p / c_v$$, the specific heat ratio).

The system (15) can be rewritten in vector form

(17)$\frac{\partial \bm{q}}{\partial t} + \nabla \cdot \bm{F}(\bm{q}) -S(\bm{q}) = 0 \, ,$

for the state variables 5-dimensional vector

$\bm{q} = \begin{pmatrix} \rho \\ \bm{U} \equiv \rho \bm{ u }\\ E \equiv \rho e \end{pmatrix} \begin{array}{l} \leftarrow\textrm{ volume mass density}\\ \leftarrow\textrm{ momentum density}\\ \leftarrow\textrm{ energy density} \end{array}$

where the flux and the source terms, respectively, are given by

\begin{aligned} \bm{F}(\bm{q}) &= \begin{pmatrix} \bm{U}\\ {(\bm{U} \otimes \bm{U})}/{\rho} + P \bm{I}_3 - \bm{\sigma} \\ {(E + P)\bm{U}}/{\rho} - \bm{u} \cdot \bm{\sigma} - k \nabla T \end{pmatrix} ,\\ S(\bm{q}) &= - \begin{pmatrix} 0\\ \rho g \bm{\hat{k}}\\ 0 \end{pmatrix}. \end{aligned}

Let the discrete solution be

$\bm{q}_N (\bm{x},t)^{(e)} = \sum_{k=1}^{P}\psi_k (\bm{x})\bm{q}_k^{(e)}$

with $$P=p+1$$ the number of nodes in the element $$e$$. We use tensor-product bases $$\psi_{kji} = h_i(X_0)h_j(X_1)h_k(X_2)$$.

For the time discretization, we use two types of time stepping schemes.

• Explicit time-stepping method

The following explicit formulation is solved with the adaptive Runge-Kutta-Fehlberg (RKF4-5) method by default (any explicit time-stepping scheme available in PETSc can be chosen at runtime)

$\bm{q}_N^{n+1} = \bm{q}_N^n + \Delta t \sum_{i=1}^{s} b_i k_i \, ,$

where

\begin{aligned} k_1 &= f(t^n, \bm{q}_N^n)\\ k_2 &= f(t^n + c_2 \Delta t, \bm{q}_N^n + \Delta t (a_{21} k_1))\\ k_3 &= f(t^n + c_3 \Delta t, \bm{q}_N^n + \Delta t (a_{31} k_1 + a_{32} k_2))\\ \vdots&\\ k_i &= f\left(t^n + c_i \Delta t, \bm{q}_N^n + \Delta t \sum_{j=1}^s a_{ij} k_j \right)\\ \end{aligned}

and with

$f(t^n, \bm{q}_N^n) = - [\nabla \cdot \bm{F}(\bm{q}_N)]^n + [S(\bm{q}_N)]^n \, .$
• Implicit time-stepping method

This time stepping method which can be selected using the option -implicit is solved with Backward Differentiation Formula (BDF) method by default (similarly, any implicit time-stepping scheme available in PETSc can be chosen at runtime). The implicit formulation solves nonlinear systems for $$\bm q_N$$:

(18)$\bm f(\bm q_N) \equiv \bm g(t^{n+1}, \bm{q}_N, \bm{\dot{q}}_N) = 0 \, ,$

where the time derivative $$\bm{\dot q}_N$$ is defined by

$\bm{\dot{q}}_N(\bm q_N) = \alpha \bm q_N + \bm z_N$

in terms of $$\bm z_N$$ from prior state and $$\alpha > 0$$, both of which depend on the specific time integration scheme (backward difference formulas, generalized alpha, implicit Runge-Kutta, etc.). Each nonlinear system (18) will correspond to a weak form, as explained below. In determining how difficult a given problem is to solve, we consider the Jacobian of (18),

$\frac{\partial \bm f}{\partial \bm q_N} = \frac{\partial \bm g}{\partial \bm q_N} + \alpha \frac{\partial \bm g}{\partial \bm{\dot q}_N}.$

The scalar “shift” $$\alpha$$ scales inversely with the time step $$\Delta t$$, so small time steps result in the Jacobian being dominated by the second term, which is a sort of “mass matrix”, and typically well-conditioned independent of grid resolution with a simple preconditioner (such as Jacobi). In contrast, the first term dominates for large time steps, with a condition number that grows with the diameter of the domain and polynomial degree of the approximation space. Both terms are significant for time-accurate simulation and the setup costs of strong preconditioners must be balanced with the convergence rate of Krylov methods using weak preconditioners.

To obtain a finite element discretization, we first multiply the strong form (17) by a test function $$\bm v \in H^1(\Omega)$$ and integrate,

$\int_{\Omega} \bm v \cdot \left(\frac{\partial \bm{q}_N}{\partial t} + \nabla \cdot \bm{F}(\bm{q}_N) - \bm{S}(\bm{q}_N) \right) \,dV = 0 \, , \; \forall \bm v \in \mathcal{V}_p\,,$

with $$\mathcal{V}_p = \{ \bm v(\bm x) \in H^{1}(\Omega_e) \,|\, \bm v(\bm x_e(\bm X)) \in P_p(\bm{I}), e=1,\ldots,N_e \}$$ a mapped space of polynomials containing at least polynomials of degree $$p$$ (with or without the higher mixed terms that appear in tensor product spaces).

Integrating by parts on the divergence term, we arrive at the weak form,

(19)\begin{aligned} \int_{\Omega} \bm v \cdot \left( \frac{\partial \bm{q}_N}{\partial t} - \bm{S}(\bm{q}_N) \right) \,dV - \int_{\Omega} \nabla \bm v \!:\! \bm{F}(\bm{q}_N)\,dV & \\ + \int_{\partial \Omega} \bm v \cdot \bm{F}(\bm q_N) \cdot \widehat{\bm{n}} \,dS &= 0 \, , \; \forall \bm v \in \mathcal{V}_p \,, \end{aligned}

where $$\bm{F}(\bm q_N) \cdot \widehat{\bm{n}}$$ is typically replaced with a boundary condition.

Note

The notation $$\nabla \bm v \!:\! \bm F$$ represents contraction over both fields and spatial dimensions while a single dot represents contraction in just one, which should be clear from context, e.g., $$\bm v \cdot \bm S$$ contracts over fields while $$\bm F \cdot \widehat{\bm n}$$ contracts over spatial dimensions.

We solve (19) using a Galerkin discretization (default) or a stabilized method, as is necessary for most real-world flows.

Galerkin methods produce oscillations for transport-dominated problems (any time the cell Péclet number is larger than 1), and those tend to blow up for nonlinear problems such as the Euler equations and (low-viscosity/poorly resolved) Navier-Stokes, in which case stabilization is necessary. Our formulation follows [HST10], which offers a comprehensive review of stabilization and shock-capturing methods for continuous finite element discretization of compressible flows.

• SUPG (streamline-upwind/Petrov-Galerkin)

In this method, the weighted residual of the strong form (17) is added to the Galerkin formulation (19). The weak form for this method is given as

(20)\begin{aligned} \int_{\Omega} \bm v \cdot \left( \frac{\partial \bm{q}_N}{\partial t} - \bm{S}(\bm{q}_N) \right) \,dV - \int_{\Omega} \nabla \bm v \!:\! \bm{F}(\bm{q}_N)\,dV & \\ + \int_{\partial \Omega} \bm v \cdot \bm{F}(\bm{q}_N) \cdot \widehat{\bm{n}} \,dS & \\ + \int_{\Omega} \bm{P}(\bm v)^T \, \left( \frac{\partial \bm{q}_N}{\partial t} \, + \, \nabla \cdot \bm{F} \, (\bm{q}_N) - \bm{S}(\bm{q}_N) \right) \,dV &= 0 \, , \; \forall \bm v \in \mathcal{V}_p \end{aligned}

This stabilization technique can be selected using the option -stab supg.

• SU (streamline-upwind)

This method is a simplified version of SUPG (20) which is developed for debugging/comparison purposes. The weak form for this method is

(21)\begin{aligned} \int_{\Omega} \bm v \cdot \left( \frac{\partial \bm{q}_N}{\partial t} - \bm{S}(\bm{q}_N) \right) \,dV - \int_{\Omega} \nabla \bm v \!:\! \bm{F}(\bm{q}_N)\,dV & \\ + \int_{\partial \Omega} \bm v \cdot \bm{F}(\bm{q}_N) \cdot \widehat{\bm{n}} \,dS & \\ + \int_{\Omega} \bm{P}(\bm v)^T \, \nabla \cdot \bm{F} \, (\bm{q}_N) \,dV & = 0 \, , \; \forall \bm v \in \mathcal{V}_p \end{aligned}

This stabilization technique can be selected using the option -stab su.

In both (21) and (20), $$\bm{P} \,$$ is called the perturbation to the test-function space, since it modifies the original Galerkin method into SUPG or SU schemes. It is defined as

$\bm{P}(\bm v) \equiv \left(\bm{\tau} \cdot \frac{\partial \bm{F} \, (\bm{q}_N)}{\partial \bm{q}_N} \right)^T \, \nabla \bm v\,,$

where parameter $$\bm{\tau} \in \mathbb R^{3\times 3}$$ is an intrinsic time/space scale matrix.

Currently, this demo provides three types of problems/physical models that can be selected at run time via the option -problem. , the problem of the transport of energy in a uniform vector velocity field, , the exact solution to the Euler equations, and the so called problem.

A simplified version of system (15), only accounting for the transport of total energy, is given by

(22)$\frac{\partial E}{\partial t} + \nabla \cdot (\bm{u} E ) = 0 \, ,$

with $$\bm{u}$$ the vector velocity field. In this particular test case, a blob of total energy (defined by a characteristic radius $$r_c$$) is transported by two different wind types.

• Rotation

In this case, a uniform circular velocity field transports the blob of total energy. We have solved (22) applying zero energy density $$E$$, and no-flux for $$\bm{u}$$ on the boundaries.

The $$3D$$ version of this test case can be run with:

./navierstokes -problem advection -wind_type rotation


while the $$2D$$ version with:

./navierstokes -problem advection2d -wind_type rotation

• Translation

In this case, a background wind with a constant rectilinear velocity field, enters the domain and transports the blob of total energy out of the domain.

For the inflow boundary conditions, a prescribed $$E_{wind}$$ is applied weakly on the inflow boundaries such that the weak form boundary integral in (19) is defined as

$\int_{\partial \Omega_{inflow}} \bm v \cdot \bm{F}(\bm q_N) \cdot \widehat{\bm{n}} \,dS = \int_{\partial \Omega_{inflow}} \bm v \, E_{wind} \, \bm u \cdot \widehat{\bm{n}} \,dS \, ,$

For the outflow boundary conditions, we have used the current values of $$E$$, following [PMK92] which extends the validity of the weak form of the governing equations to the outflow instead of replacing them with unknown essential or natural boundary conditions. The weak form boundary integral in (19) for outflow boundary conditions is defined as

$\int_{\partial \Omega_{outflow}} \bm v \cdot \bm{F}(\bm q_N) \cdot \widehat{\bm{n}} \,dS = \int_{\partial \Omega_{outflow}} \bm v \, E \, \bm u \cdot \widehat{\bm{n}} \,dS \, ,$

The $$3D$$ version of this test case problem can be run with:

./navierstokes -problem advection -wind_type translation -wind_translation .5,-1,0


while the $$2D$$ version with:

./navierstokes -problem advection2d -wind_type translation -wind_translation 1,-.5


## Isentropic Vortex¶

Three-dimensional Euler equations, which are simplified version of system (15) and account only for the convective fluxes, are given by

(23)\begin{aligned} \frac{\partial \rho}{\partial t} + \nabla \cdot \bm{U} &= 0 \\ \frac{\partial \bm{U}}{\partial t} + \nabla \cdot \left( \frac{\bm{U} \otimes \bm{U}}{\rho} + P \bm{I}_3 \right) &= 0 \\ \frac{\partial E}{\partial t} + \nabla \cdot \left( \frac{(E + P)\bm{U}}{\rho} \right) &= 0 \, , \\ \end{aligned}

Following the setup given in [ZZS11], the mean flow for this problem is $$\rho=1$$, $$P=1$$, $$T=P/\rho= 1$$, and $$\bm{u}=(u_1,u_2,0)$$ while the perturbation $$\delta \bm{u}$$, and $$\delta T$$ are defined as

\begin{aligned} (\delta u_1, \, \delta u_2) &= \frac{\epsilon}{2 \pi} \, e^{0.5(1-r^2)} \, (-\bar{y}, \, \bar{x}) \, , \\ \delta T &= - \frac{(\gamma-1) \, \epsilon^2}{8 \, \gamma \, \pi^2} \, e^{1-r^2} \, , \\ \end{aligned}

where $$(\bar{x}, \, \bar{y}) = (x-x_c, \, y-y_c)$$, $$(x_c, \, y_c)$$ represents the center of the domain, $$r^2=\bar{x}^2 + \bar{y}^2$$, and $$\epsilon$$ is the vortex strength. There is no perturbation in the entropy $$S=P/\rho^\gamma$$ ($$\delta S=0)$$.

This problem can be run with:

./navierstokes -problem euler_vortex -mean_velocity .5,-.8,0.


## Density Current¶

For this test problem (from [SWW+93]), we solve the full Navier-Stokes equations (15), for which a cold air bubble (of radius $$r_c$$) drops by convection in a neutrally stratified atmosphere. Its initial condition is defined in terms of the Exner pressure, $$\pi(\bm{x},t)$$, and potential temperature, $$\theta(\bm{x},t)$$, that relate to the state variables via

\begin{aligned} \rho &= \frac{P_0}{( c_p - c_v)\theta(\bm{x},t)} \pi(\bm{x},t)^{\frac{c_v}{ c_p - c_v}} \, , \\ e &= c_v \theta(\bm{x},t) \pi(\bm{x},t) + \bm{u}\cdot \bm{u} /2 + g z \, , \end{aligned}

where $$P_0$$ is the atmospheric pressure. For this problem, we have used no-slip and non-penetration boundary conditions for $$\bm{u}$$, and no-flux for mass and energy densities. This problem can be run with:

./navierstokes -problem density_current