Author: Riccardo Tosi
Kratos version: 8.0
Source files: source
This example is taken from [Donea, J., & Huerta, A. (2003). Finite Element Methods for Flow Problems. Section 5.6.2]. We solve the transient convection diffusion equation , where null Dirichlet boundary condition and null initial conditions are set. We refer to the above reference for further details.
Citing [Donea, J., & Huerta, A. (2003). Finite Element Methods for Flow Problems. Section 5.6.2], this problem requires accurate transport of the unknown and boundary layers appear in the solution due to the Dirichlet boundary conditions. Therefore, high-order time-stepping schemes and stabilized formulations are needed in order to obtain an accurate solution.
The problem is solved exploiting the Runge-Kutta 4 time integration explicit method, and it can be run with four different stabilizations:
- quasi-static algebraic subgrid scale (QSASGS)
- quasi-static orthogonal subgrid scale (QSOSS)
- dynamic algebraic subgrid scale (DASGS)
- dynamic orthogonal subgrid scale (DOSS)
We present the temporal evolution of for the DOSS case.
We can observe that the results we obtain are consistent with the reference [Donea, J., & Huerta, A. (2003). Finite Element Methods for Flow Problems. Section 5.6.2].