# CFL condition in Stokes equation

Does the CFL condition play any role in a pure Stokes flow, i.e. convective term is neglibile, or vanishing? If not, what is the "equivalent" condition for stability? I have read something about the diffusional time scale but it's quite vague. Anyone with in-depth insight?

And a quotation from a paper :
"The time step is $3.10^-3\dot\gamma^-1$, corresponding to a CFL number based on the diffusional time scale $CFL_d=v\Delta t/\Delta^2$ of 50."

 Gallier, S., Lemaire, E., Lobry, L., & Peters, F. (2014). A fictitious domain approach for the simulation of dense suspensions. Journal of Computational Physics, 256, 367-387.

• Do you mean the time-dependent Stokes equation? It would be useful to state the exact problem you are considering. Oct 3 '17 at 0:06
• @WolfgangBangerth I will clarify! I mean in the flow regime that the Navier stokes equations reduce to the Stokes equation: $\mu\nabla^2\mathbf{u}-\nabla p=0$ Oct 3 '17 at 4:44
• But there is no time dependence here. The CFL condition relates the time step size to the mesh size -- but you don't have a time step here. Oct 3 '17 at 17:21
• @WolfgangBangerth Although it is evident that this not apply in the steady case, does it apply in the unsteady case? $$\mu \nabla^2 \mathbf{u}- \nabla p = \frac{\partial \rho \mathbf{u}} {\partial{t}}$$ Generally we would solve the diffusion operator with an implicit scheme, so I don't think you would get a CFL in this condition no?
– BlaB
Oct 3 '17 at 20:11
• In the time dependent case, if you use an implicit time stepping scheme, then the CFL stability condition does not apply. If you use an explicit time stepping scheme, then a variation of the condition applies indeed. Oct 3 '17 at 21:25

Essentially, the time dependent Stokes equation looks like the heat equation: $$\frac{\partial u}{\partial t} - \nu\Delta u = f-\nabla p,$$ plus the incompressibility condition $\nabla \cdot u=0$ that for the current discussion is immaterial. Thus, the same considerations for time step choice apply as for the heat equation.
On the other hand, for an explicit method, you need to choose the time step $\Delta t$ subject to some CFL-like condition that says that $$\Delta t \le C \frac{1}{\nu} \Delta x^2$$ where $\Delta x$ is the mesh size. This is not practical: it requires you to choose the time step four times smaller for each mesh refinement. These time steps would be so small that the time discretization error is vastly smaller than the spatial discretization error, and that's not useful. As a consequence, practical implementations do not choose explicit methods for the Stokes equation.