In this section we will perform a transient growth analysis of the flow over a backward-facing step. This is an important case which allows us to understand the effects of separation due to abrupt changes of geometry in an open flow. The transient growth analysis consists of computing the maximum energy growth, G(τ), attainable over all possible initial conditions u′(0) for a specified time horizon τ. It can be demonstrated that it is equivalent to calculating the largest eigenvalue of ∗(τ)(τ), with and ∗ being the direct and the adjoint operators, respectively. Also note that the eigenvalue must necessarily be real since ∗(τ)(τ) is self-adjoint in this case.
The files for this section can be found in the $NEKTUTORIAL/BackwardStep
directory.
Geometry
bfs.geo
- Gmsh file that contains the geometry of the problem
bfs.msh
- Gmsh generated mesh data listing mesh vertices and elements.Base
bfs-Base.xml
- Nektar++ session file, generated with the $NEK/MeshConvert
utility, for
computing the base flow.
bfs-Base.fld
- Nektar++ field file that contains the base flow, generated using bfs-Base.xml
.Stability
bfs_tg.xml
- Nektar++ session file, generated with $NEK/MeshConvert
, for performing
the transient growth analysis.
bfs_tg.bse
- Nektar++ field file that contains the base flow. It is the same as the .fld
file present in the folder Base
.Figure 4 shows the mesh, along with a detailed view of the step edge, that we will use for the
computation. The geometry is non-dimensionalised by the step height. The domain has an
inflow length of 10 upstream of the step edge and a downstream channel of length 50. The mesh
consist of N = 430 elements. Note that in this case the mesh is composed of both triangular
and quadrilateral elements. A refined triangular unstructured mesh is used near the step to
capture the separation effects, whereas the inflow/outflow channels have a structure similar to the
previous example. Therefore in the EXPANSION
section of the bfs-Base.xml
file, two composites
(C[0]
and C[1]
) are present. For this example, we will use the modal basis with 7th-order
polynomials.
We will perform simulations at Re = 500, since it is well-known that for this value the flow presents a strong convective instability.