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Fix typos in template, changed streamwise readme a bit.
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# Streamwise Periodicity testcases
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All Testcases use the incompressible solver implemented by Thomas Economon.
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For all Testcases the respective gmsh geo file has to be provided.
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This folder contains the additional Testcases for streamwise periodic flow.
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A Tutorial can be found on the SU2 website.
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For all Testcases a gmsh .geo file is provided which allows to recreate/modify the mesh.
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## `pipe_slice_3D`
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## `pipe_slice_3d`
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Overview: Hagen Poiseuille flow through a 1-primal-cell thick pipe slice in 3D.
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Hagen Poiseuille flow through a 1-primal-cell thick pipe slice in 3D.
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Analytical solution of the velocity magnitude for steady laminar pipe flow in a round pipe `v_mag (r) = -1/(4*mu) * (Delta p / Delta x) * (R**2 - r**2)` therefore a pressure drop Delta p is prescribed, heated walls
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Analytical solution of the velocity magnitude for steady laminar pipe flow in a round pipe `v_mag (r) = -1/(4*mu) * (Delta p / Delta x) * (R**2 - r**2)` therefore a pressure drop Delta p is prescribed.
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`Re = rho * v * L / mu = 1.0 * ? * 5e-3 / 1.8e-5` bei v -> averaged (mass or area weighted?) velocity the critical Re ~= 2300 (v = 0.6 for now) makes Re=167
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`Re = rho * v * L / mu = 1.0 * 0.6 * 5e-3 / 1.8e-5` makes Re=167, with the critical Reynolds number being Re~=2300.
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It would nice to have a Re ~= 1500 to have a better testcase (achieve that with v~5 or 6 i.e. scale Delta P by factor 10 from 0.001 to 0.01)
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This testcase is a regression test.
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## `half_cylinder_2D`
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half cylinder massflow prescribed heated cylinder - probably discontinued
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## `chtPinArray_2d`
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## 2D_pinArray_dp_hf
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Extension of the tutorial case to a CHT problem with 1 additional solid zone.
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A gradient validation between discrete and finite differences for this setup is described in the README of that folder.
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## 2D_pinArray_mf
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This gradient validation is also part of the regression tests.
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## 2D_pinArray_cht_dp_hf
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## `chtPinArray_3d`
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### Discrete Adjoint
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Extension of the `chtPinArray_2d` to the 3rd dimension with again one solid zone.
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The mesh provided is coarse to keep the filesize and computation time low, but using the gmsh .geo script much higher mesh resolutions can be created.
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## 3D_pinArray_mf_hf
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## 3D_pinArray_cht_dp_hf
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### Discrete Adjoint
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This primal simulation is part of the regression tests.

config_template.cfg

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% --------------------- STREAMWISE PERIODICITY DEFINITION ---------------------%
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%
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% Generally for streamwise periodicty one has to set MARKER_PERIODIC= (<inlet>, <outlet>, ...)
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% appropriatley as a boundary condition.
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% Generally for streamwise periodictiy one has to set MARKER_PERIODIC= (<inlet>, <outlet>, ...)
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% appropriately as a boundary condition.
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%
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% Specify type of streamwise periodicty (default=NONE, PRESSURE_DROP, MASSFLOW)
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% Specify type of streamwise periodictiy (default=NONE, PRESSURE_DROP, MASSFLOW)
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KIND_STREAMWISE_PERIODIC= NONE
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%
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% Delta P [Pa] value that drives the flow as a source term in the momentum equations.
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STREAMWISE_PERIODIC_MASSFLOW= 0.0
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%
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% Use streamwise periodic temperature (default=NO, YES)
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% If YES, the heatflux is taken out at the outlet
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% If NO, the heatflux is taken out at the outlet.
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% This option is only necessary if INC_ENERGY_EQUATION=YES
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STREAMWISE_PERIODIC_TEMPERATURE= NO
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%
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% Prescibe integrated heat [W] extracted at the periodic "outlet".
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% Prescribe integrated heat [W] extracted at the periodic "outlet".
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% Only active if STREAMWISE_PERIODIC_TEMPERATURE= NO.
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% If set to zero, the heat is integrated automatically over all present MARKER_HEATFLUX.
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% Upon convergence, the area averaged inlet temperature will be INC_TEMPERATURE_INIT.

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