Two-dimensional channel flow
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Geometry of a two-dimensional channel flow.
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The Orr-Sommerfeld equation governs the dynamics of two-dimensional velocity
fluctuations around the laminar channel flow,
where
| — | streamfunction |
| — | Reynolds number |
| — | streamwise wavenumber |
| — | wall-normal coordinate |
| — | base flow |
| — | Laplacian |
| — | ‘‘square’’ of the Laplacian |
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For (based on the centerline velocity and
the channel half-width), the discretized version of the Orr-Sommerfeld
equation is obtained using the pseudo-spectral scheme with
colocation points in the wall-normal direction. Flow fluctuations with
are then advanced in time using the matrix exponential with
time step and randomly generated initial profile (that
satisfies both homogeneous Dirichlet and Neumann boundary conditions).
After a transient period of ten time-steps, snapshots are
taken to form the snapshot matrices and apply the standard DMD algorithm
along with its sparsity-promoting variant.
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