From c956976644adc84deb0c23a02ecac5a0e6d717d2 Mon Sep 17 00:00:00 2001
From: marchdf where \(\Omega\) is the earth’s angular velocity and \(\lambda\) is the latitude. To account for the effects of the laminar-turbulent boundary layer transition,
+Menter’s one-equation \(\gamma\) transition model :cite:`Menter:2015` is coupled with the SST model.
+The model consists of single transport equation for intermittency The production term, \(P_{\gamma}\), and destruction term, \(D_{\gamma}\), are as: The model constants are: The transition onset criteria of the model are defined as: The transition onset occurs once the scaled vorticity Reynolds number, \(Re_{v}/2.2\), exceeds the critical momentum thickness Reynolds number, \(Re_{\theta c}\), from the empirical correlations. The output intermittency from the transition model is applied to both the production and destruction terms of the turbulent kinetic energy
+transport equation. The DES technique is also supported in the code base when the SST model
is activated. This model seeks to formally relax the RANS-based approach
and allows for a theoretical basis to allow for transient flows. The
method follows the method of Temporally Filtered NS formulation as
-described by Tieszen, :cite:`Tieszen:2005`.
+
+
+
+
+
+
+
+ #include "node_kernels/SDRSSTBLTM2015NodeKernel.h"
+#include "Realm.h"
+#include "SolutionOptions.h"
+#include "SimdInterface.h"
+#include "utils/StkHelpers.h"
+#include "stk_mesh/base/MetaData.hpp"
+#include "stk_mesh/base/Types.hpp"
+
+
+
+
+Namespaces
+ sierra
+
+ sierra::nalu
+
+Generated by 1.9.1
+
+
+
diff --git a/api_docs/_s_d_r_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.map b/api_docs/_s_d_r_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.map
new file mode 100644
index 000000000..66508b7a0
--- /dev/null
+++ b/api_docs/_s_d_r_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.map
@@ -0,0 +1,10 @@
+
diff --git a/api_docs/_s_d_r_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.md5 b/api_docs/_s_d_r_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.md5
new file mode 100644
index 000000000..e8978c2bd
--- /dev/null
+++ b/api_docs/_s_d_r_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.md5
@@ -0,0 +1 @@
+1458bbe6fcfefadd5aa2b5c09aa37c1a
\ No newline at end of file
diff --git a/api_docs/_s_d_r_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.svg b/api_docs/_s_d_r_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.svg
new file mode 100644
index 000000000..23807f199
--- /dev/null
+++ b/api_docs/_s_d_r_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.svg
@@ -0,0 +1,216 @@
+
+
+
+
+
+
diff --git a/api_docs/_s_d_r_s_s_t_b_l_t_m2015_node_kernel_8_c__incl_org.svg b/api_docs/_s_d_r_s_s_t_b_l_t_m2015_node_kernel_8_c__incl_org.svg
new file mode 100644
index 000000000..8734d8b4b
--- /dev/null
+++ b/api_docs/_s_d_r_s_s_t_b_l_t_m2015_node_kernel_8_c__incl_org.svg
@@ -0,0 +1,128 @@
+
+
+
+
+#include <node_kernels/SDRSSTDESNodeKernel.h>
#include <node_kernels/ScalarGclNodeKernel.h>
#include <node_kernels/SDRKONodeKernel.h>
+#include <node_kernels/SDRSSTBLTM2015NodeKernel.h>
#include "ngp_utils/NgpFieldBLAS.h"
#include "ngp_algorithms/NodalGradEdgeAlg.h"
#include "ngp_algorithms/NodalGradElemAlg.h"
diff --git a/api_docs/_t_k_e_s_s_t_b_l_t_m2015_node_kernel_8_c.html b/api_docs/_t_k_e_s_s_t_b_l_t_m2015_node_kernel_8_c.html
new file mode 100644
index 000000000..31ee81830
--- /dev/null
+++ b/api_docs/_t_k_e_s_s_t_b_l_t_m2015_node_kernel_8_c.html
@@ -0,0 +1,110 @@
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+ #include "node_kernels/TKESSTBLTM2015NodeKernel.h"
+#include "Realm.h"
+#include "SolutionOptions.h"
+#include "SimdInterface.h"
+#include "utils/StkHelpers.h"
+#include "stk_mesh/base/MetaData.hpp"
+#include "stk_mesh/base/Types.hpp"
+
+
+
+
+Namespaces
+ sierra
+
+ sierra::nalu
+
+Generated by 1.9.1
+
+
+
diff --git a/api_docs/_t_k_e_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.map b/api_docs/_t_k_e_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.map
new file mode 100644
index 000000000..b9eb8772e
--- /dev/null
+++ b/api_docs/_t_k_e_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.map
@@ -0,0 +1,10 @@
+
diff --git a/api_docs/_t_k_e_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.md5 b/api_docs/_t_k_e_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.md5
new file mode 100644
index 000000000..93ea637b9
--- /dev/null
+++ b/api_docs/_t_k_e_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.md5
@@ -0,0 +1 @@
+2333187576f145e078d519ab1c1f3001
\ No newline at end of file
diff --git a/api_docs/_t_k_e_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.svg b/api_docs/_t_k_e_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.svg
new file mode 100644
index 000000000..8d6601646
--- /dev/null
+++ b/api_docs/_t_k_e_s_s_t_b_l_t_m2015_node_kernel_8_c__incl.svg
@@ -0,0 +1,216 @@
+
+
+
+
+
+#include <node_kernels/TKEKENodeKernel.h>
#include <node_kernels/TKERodiNodeKernel.h>
#include <node_kernels/TKEKONodeKernel.h>
+#include <node_kernels/TKESSTBLTM2015NodeKernel.h>
#include <ngp_utils/NgpLoopUtils.h>
#include <ngp_utils/NgpTypes.h>
#include <ngp_utils/NgpFieldBLAS.h>
diff --git a/api_docs/dir_e472670134093ca813a7551919ab9780.html b/api_docs/dir_e472670134093ca813a7551919ab9780.html
index bb5026874..1f7a1fd56 100644
--- a/api_docs/dir_e472670134093ca813a7551919ab9780.html
+++ b/api_docs/dir_e472670134093ca813a7551919ab9780.html
@@ -117,6 +117,8 @@
file SDRSSTAMSNodeKernel.C
+
+file SDRSSTBLTM2015NodeKernel.C file SDRSSTDESNodeKernel.C
@@ -135,6 +137,8 @@
file SDRSSTLRNodeKernel.C file TKESSTAMSNodeKernel.C
+
+file TKESSTBLTM2015NodeKernel.C file TKESSTDESNodeKernel.C
diff --git a/api_docs/files.html b/api_docs/files.html
index d130056c1..96544a8d1 100644
--- a/api_docs/files.html
+++ b/api_docs/files.html
@@ -363,124 +363,126 @@
file TKESSTIDDESNodeKernel.C SDRKONodeKernel.C SDRLowReWallAlg.C
- SDRSSTAMSNodeKernel.C
- SDRSSTDESNodeKernel.C
- SDRSSTLRNodeKernel.C
- SDRSSTNodeKernel.C
- SDRWallFuncAlg.C
- SDRWallFuncAlgDriver.C
- ShearStressTransportEquationSystem.C
- SideWriter.C
- Simulation.C
- SinProfileChannelFlowVelocityAuxFunction.C
- SloshingTankVOFAuxFunction.C
- SmartField.C
- SolutionNormPostProcessing.C
- SolutionOptions.C
- SolverAlgorithm.C
- SolverAlgorithmDriver.C
- SparsifiedEdgeLaplacian.C
- SpecificDissipationRateEquationSystem.C
- SpecificHeatPropertyEvaluator.C
- SSTAMSAveragesAlg.C
- SSTMaxLengthScaleAlg.C
- SSTMaxLengthScaleDriver.C
- SteadyTaylorVortexGradPressureAuxFunction.C
- SteadyTaylorVortexMomentumSrcNodeSuppAlg.C
- SteadyTaylorVortexPressureAuxFunction.C
- SteadyTaylorVortexVelocityAuxFunction.C
- StkHelpers.C
- StkSimdConnectivityMap.C
- StkSimdFaceConnectivityMap.C
- StkSimdGatheredElementData.C
- StkSimdNodeConnectivityMap.C
- StkToTpetraComm.C
- StkToTpetraLocalIndices.C
- StkToTpetraMap.C
- StreletsUpwindEdgeAlg.C
- StringTimeCoordFunction.C
- StringTimeCoordTemperatureAuxFunction.C
- StrongDirichletBC.C
- SupplementalAlgorithm.C
- SurfaceForceAndMomentAlgorithm.C
- SurfaceForceAndMomentAlgorithmDriver.C
- SurfaceForceAndMomentWallFunctionAlgorithm.C
- SutherlandsPropertyEvaluator.C
- SyntheticLidar.C
- TabulatedTemperatureAuxFunction.C
- TaylorGreenPressureAuxFunction.C
- TaylorGreenVelocityAuxFunction.C
- TDRKENodeKernel.C
- TemperaturePropAlgorithm.C
- Tet4CVFEM.C
- ThermalConductivityFromPrandtlPropAlgorithm.C
- TimeIntegrator.C
- TiogaBlock.C
- TiogaOptions.C
- TiogaRef.C
- TiogaSTKIface.C
- TKEKENodeKernel.C
- TKEKONodeKernel.C
- TKEKsgsNodeKernel.C
- TKERodiNodeKernel.C
- TKESSTAMSNodeKernel.C
- TKESSTDESNodeKernel.C
- TKESSTIDDESNodeKernel.C
- TKESSTLRNodeKernel.C
- TKESSTNodeKernel.C
- TKEWallFuncAlg.C
- TKEWallFuncAlgDriver.C
- TornadoAuxFunction.C
- TotalDissipationRateEquationSystem.C
- TpetraLinearSystem.C
- TpetraLinearSystemHelpers.C
- TpetraSegregatedLinearSystem.C
- Transfer.C
- Transfers.C
- TransportCoefficients.C
- Tri32DCVFEM.C
- Tri33DCVFEM.C
- TurbineSurrogateKernel.C
- TurbKineticEnergyEquationSystem.C
- TurbulenceAveragingPostProcessing.C
- TurbViscKEAlg.C
- TurbViscKOAlg.C
- TurbViscKsgsAlg.C
- TurbViscSmagorinskyAlgorithm.C
- TurbViscSSTAlg.C
- TurbViscSSTLRAlg.C
- TurbViscWaleAlgorithm.C
- UpdateOversetFringeAlgorithmDriver.C
- UtilitiesActuator.C
- VariableDensityContinuitySrcNodeSuppAlg.C
- VariableDensityMixFracAuxFunction.C
- VariableDensityMixFracSrcNodeSuppAlg.C
- VariableDensityMomentumSrcNodeSuppAlg.C
- VariableDensityNonIsoContinuitySrcNodeSuppAlg.C
- VariableDensityNonIsoEnthalpySrcNodeSuppAlg.C
- VariableDensityNonIsoMomentumSrcNodeSuppAlg.C
- VariableDensityNonIsoTemperatureAuxFunction.C
- VariableDensityPressureAuxFunction.C
- VariableDensityVelocityAuxFunction.C
- VOFAdvectionEdgeAlg.C
- VOFGclNodeKernel.C
- VOFMassBDFNodeKernel.C
- VolumeOfFluidEquationSystem.C
- WallDistEdgeSolverAlg.C
- WallDistElemKernel.C
- WallDistEquationSystem.C
- WallDistNodeKernel.C
- WallFricVelAlgDriver.C
- WallFuncGeometryAlg.C
- WaterPropertyEvaluator.C
- Wed6CVFEM.C
- WilcoxKOmegaEquationSystem.C
- WindEnergyPowerLawAuxFunction.C
- WindEnergyTaylorVortexAuxFunction.C
- WindEnergyTaylorVortexPressureAuxFunction.C
- ZalesakDiskMassFlowRateKernel.C
- ZalesakDiskVOFAuxFunction.C
- ZalesakSphereMassFlowRateKernel.C
+ ZalesakSphereVOFAuxFunction.C
+ SDRSSTBLTM2015NodeKernel.C
+ SDRSSTDESNodeKernel.C
+ SDRSSTLRNodeKernel.C
+ SDRSSTNodeKernel.C
+ SDRWallFuncAlg.C
+ SDRWallFuncAlgDriver.C
+ ShearStressTransportEquationSystem.C
+ SideWriter.C
+ Simulation.C
+ SinProfileChannelFlowVelocityAuxFunction.C
+ SloshingTankVOFAuxFunction.C
+ SmartField.C
+ SolutionNormPostProcessing.C
+ SolutionOptions.C
+ SolverAlgorithm.C
+ SolverAlgorithmDriver.C
+ SparsifiedEdgeLaplacian.C
+ SpecificDissipationRateEquationSystem.C
+ SpecificHeatPropertyEvaluator.C
+ SSTAMSAveragesAlg.C
+ SSTMaxLengthScaleAlg.C
+ SSTMaxLengthScaleDriver.C
+ SteadyTaylorVortexGradPressureAuxFunction.C
+ SteadyTaylorVortexMomentumSrcNodeSuppAlg.C
+ SteadyTaylorVortexPressureAuxFunction.C
+ SteadyTaylorVortexVelocityAuxFunction.C
+ StkHelpers.C
+ StkSimdConnectivityMap.C
+ StkSimdFaceConnectivityMap.C
+ StkSimdGatheredElementData.C
+ StkSimdNodeConnectivityMap.C
+ StkToTpetraComm.C
+ StkToTpetraLocalIndices.C
+ StkToTpetraMap.C
+ StreletsUpwindEdgeAlg.C
+ StringTimeCoordFunction.C
+ StringTimeCoordTemperatureAuxFunction.C
+ StrongDirichletBC.C
+ SupplementalAlgorithm.C
+ SurfaceForceAndMomentAlgorithm.C
+ SurfaceForceAndMomentAlgorithmDriver.C
+ SurfaceForceAndMomentWallFunctionAlgorithm.C
+ SutherlandsPropertyEvaluator.C
+ SyntheticLidar.C
+ TabulatedTemperatureAuxFunction.C
+ TaylorGreenPressureAuxFunction.C
+ TaylorGreenVelocityAuxFunction.C
+ TDRKENodeKernel.C
+ TemperaturePropAlgorithm.C
+ Tet4CVFEM.C
+ ThermalConductivityFromPrandtlPropAlgorithm.C
+ TimeIntegrator.C
+ TiogaBlock.C
+ TiogaOptions.C
+ TiogaRef.C
+ TiogaSTKIface.C
+ TKEKENodeKernel.C
+ TKEKONodeKernel.C
+ TKEKsgsNodeKernel.C
+ TKERodiNodeKernel.C
+ TKESSTAMSNodeKernel.C
+ TKESSTBLTM2015NodeKernel.C
+ TKESSTDESNodeKernel.C
+ TKESSTIDDESNodeKernel.C
+ TKESSTLRNodeKernel.C
+ TKESSTNodeKernel.C
+ TKEWallFuncAlg.C
+ TKEWallFuncAlgDriver.C
+ TornadoAuxFunction.C
+ TotalDissipationRateEquationSystem.C
+ TpetraLinearSystem.C
+ TpetraLinearSystemHelpers.C
+ TpetraSegregatedLinearSystem.C
+ Transfer.C
+ Transfers.C
+ TransportCoefficients.C
+ Tri32DCVFEM.C
+ Tri33DCVFEM.C
+ TurbineSurrogateKernel.C
+ TurbKineticEnergyEquationSystem.C
+ TurbulenceAveragingPostProcessing.C
+ TurbViscKEAlg.C
+ TurbViscKOAlg.C
+ TurbViscKsgsAlg.C
+ TurbViscSmagorinskyAlgorithm.C
+ TurbViscSSTAlg.C
+ TurbViscSSTLRAlg.C
+ TurbViscWaleAlgorithm.C
+ UpdateOversetFringeAlgorithmDriver.C
+ UtilitiesActuator.C
+ VariableDensityContinuitySrcNodeSuppAlg.C
+ VariableDensityMixFracAuxFunction.C
+ VariableDensityMixFracSrcNodeSuppAlg.C
+ VariableDensityMomentumSrcNodeSuppAlg.C
+ VariableDensityNonIsoContinuitySrcNodeSuppAlg.C
+ VariableDensityNonIsoEnthalpySrcNodeSuppAlg.C
+ VariableDensityNonIsoMomentumSrcNodeSuppAlg.C
+ VariableDensityNonIsoTemperatureAuxFunction.C
+ VariableDensityPressureAuxFunction.C
+ VariableDensityVelocityAuxFunction.C
+ VOFAdvectionEdgeAlg.C
+ VOFGclNodeKernel.C
+ VOFMassBDFNodeKernel.C
+ VolumeOfFluidEquationSystem.C
+ WallDistEdgeSolverAlg.C
+ WallDistElemKernel.C
+ WallDistEquationSystem.C
+ WallDistNodeKernel.C
+ WallFricVelAlgDriver.C
+ WallFuncGeometryAlg.C
+ WaterPropertyEvaluator.C
+ Wed6CVFEM.C
+ WilcoxKOmegaEquationSystem.C
+ WindEnergyPowerLawAuxFunction.C
+ WindEnergyTaylorVortexAuxFunction.C
+ WindEnergyTaylorVortexPressureAuxFunction.C
+ ZalesakDiskMassFlowRateKernel.C
+ ZalesakDiskVOFAuxFunction.C
+ ZalesakSphereMassFlowRateKernel.C
diff --git a/api_docs/search/all_11.js b/api_docs/search/all_11.js
index 7268dc41f..3ce34404d 100644
--- a/api_docs/search/all_11.js
+++ b/api_docs/search/all_11.js
@@ -23,74 +23,75 @@ var searchData=
['sdrkonodekernel_2ec_486',['SDRKONodeKernel.C',['../_s_d_r_k_o_node_kernel_8_c.html',1,'']]],
['sdrlowrewallalg_2ec_487',['SDRLowReWallAlg.C',['../_s_d_r_low_re_wall_alg_8_c.html',1,'']]],
['sdrsstamsnodekernel_2ec_488',['SDRSSTAMSNodeKernel.C',['../_s_d_r_s_s_t_a_m_s_node_kernel_8_c.html',1,'']]],
- ['sdrsstdesnodekernel_2ec_489',['SDRSSTDESNodeKernel.C',['../_s_d_r_s_s_t_d_e_s_node_kernel_8_c.html',1,'']]],
- ['sdrsstlrnodekernel_2ec_490',['SDRSSTLRNodeKernel.C',['../_s_d_r_s_s_t_l_r_node_kernel_8_c.html',1,'']]],
- ['sdrsstnodekernel_2ec_491',['SDRSSTNodeKernel.C',['../_s_d_r_s_s_t_node_kernel_8_c.html',1,'']]],
- ['sdrwallfuncalg_2ec_492',['SDRWallFuncAlg.C',['../_s_d_r_wall_func_alg_8_c.html',1,'']]],
- ['sdrwallfuncalgdriver_2ec_493',['SDRWallFuncAlgDriver.C',['../_s_d_r_wall_func_alg_driver_8_c.html',1,'']]],
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- ['shearstresstransportequationsystem_2ec_498',['ShearStressTransportEquationSystem.C',['../_shear_stress_transport_equation_system_8_c.html',1,'']]],
- ['shifted_5fpyr_5fderiv_499',['shifted_pyr_deriv',['../namespacesierra_1_1nalu.html#a477cfc57bed160caf9c5613600c20cb5',1,'sierra::nalu']]],
- ['sidewriter_2ec_500',['SideWriter.C',['../_side_writer_8_c.html',1,'']]],
- ['sierra_501',['sierra',['../namespacesierra.html',1,'']]],
- ['simd_5fnode_5fmap_502',['simd_node_map',['../namespacesierra_1_1nalu_1_1matrix__free.html#abf8f0341cb023a69e37eb7961b6d97ab',1,'sierra::nalu::matrix_free']]],
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- ['simulation_2ec_504',['Simulation.C',['../_simulation_8_c.html',1,'']]],
- ['sinprofilechannelflowvelocityauxfunction_2ec_505',['SinProfileChannelFlowVelocityAuxFunction.C',['../_sin_profile_channel_flow_velocity_aux_function_8_c.html',1,'']]],
- ['size_5fratio_5fx_506',['size_ratio_x',['../_perturbed_shear_layer_aux_functions_8_c.html#a9c87e5d31d7a790c0b998a4a557bda1f',1,'PerturbedShearLayerAuxFunctions.C']]],
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- ['sloshingtankvofauxfunction_2ec_509',['SloshingTankVOFAuxFunction.C',['../_sloshing_tank_v_o_f_aux_function_8_c.html',1,'']]],
- ['smartfield_2ec_510',['SmartField.C',['../_smart_field_8_c.html',1,'']]],
- ['solutionnormpostprocessing_2ec_511',['SolutionNormPostProcessing.C',['../_solution_norm_post_processing_8_c.html',1,'']]],
- ['solutionoptions_2ec_512',['SolutionOptions.C',['../_solution_options_8_c.html',1,'']]],
- ['solveralgorithm_2ec_513',['SolverAlgorithm.C',['../_solver_algorithm_8_c.html',1,'']]],
- ['solveralgorithmdriver_2ec_514',['SolverAlgorithmDriver.C',['../_solver_algorithm_driver_8_c.html',1,'']]],
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- ['sparsifiededgelaplacian_2ec_518',['SparsifiedEdgeLaplacian.C',['../_sparsified_edge_laplacian_8_c.html',1,'']]],
- ['specificdissipationrateequationsystem_2ec_519',['SpecificDissipationRateEquationSystem.C',['../_specific_dissipation_rate_equation_system_8_c.html',1,'']]],
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Nalu-Wind - Theory Manual2.8. Conservation of Species
diff --git a/source/theory/supportedEquationSet.html b/source/theory/supportedEquationSet.html
index fab3c64b8..eb09fbe76 100644
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+++ b/source/theory/supportedEquationSet.html
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-
2.10.1. Shear Stress Transport (SST) For
2.11. Laminar-Turbulent Transition Model Formulation
+2.11. Detached Eddy Simulation (DES) Formulation
+2.12. Detached Eddy Simulation (DES) Formulation
The SST DES model simply changes the turbulent kinetic energy equation to include a new minimum scale that manipulates the dissipation term.
The AMS approach is a recently developed hybrid RANS/LES framework by Haering, -Oliver and Moser :cite:`Haering-etal:2020`. In this approach a triple +Oliver and Moser :cite:`Haering-etal:2020`. In this approach a triple decomposition is used, breaking the instantaneous velocity field into an average component \(<u_i>\), a resolved fluctuation \(u_i^>\) and an unresolved fluctuation \(u_i^<\). The subgrid stress is @@ -766,13 +791,13 @@
In a typical Hybrid RANS/LES approach, the observation that the LES and RANS equations take on the same mathematical form is leveraged, relying simply on a modified turbulent viscosity coefficient that takes into account the ability to resolve some turbulent content. Due to deficiencies in this approach as discussed in Haering et -al. :cite:`Haering-etal:2020`, an alternative approach where the modeled term +al. :cite:`Haering-etal:2020`, an alternative approach where the modeled term is split into two contributions, one representing the impact on the mean flow and one the impact on the resolved fluctuations, from the unresolved content, is used in the Active Model Split (AMS) @@ -812,7 +837,7 @@
\(\tau_{ij}^{SGET}\) is modeled using the M43 SGS model discussed
-in Haering et al. :cite:`HaeringAIAA`. This uses an anisotropic
+in Haering et al. :cite:`HaeringAIAA`. This uses an anisotropic
representation, \(\tau_{ij} = \nu_{jk} \partial_k u_i + \nu_{ik}
\partial_k u_j\), of the stress tensor and a tensorial eddy viscosity,
\(\nu_{ij} = C(\mathcal{M}) \langle \epsilon \rangle^{1/3}
@@ -832,7 +857,7 @@ 2.12.1. Split subgrid model stress
The averaging algorithms are invoked as part of the AMSAlgDriver and are called from the pre_iter_work function so that they are executed at the beginning of each Picard @@ -869,7 +894,7 @@
Typically in a hybrid model, it is necessary to have diagnostics that assess the ability of the grid to resolve turbulent content and to aid in its introduction. In AMS, there are two main diagnostic @@ -901,11 +926,11 @@
When the grid is capable of resolving some turbulent content, the model will want to reduce the modeled stress and allow for resolved turbulence to contribute the remaining piece of the total stress. As -discussed in Haering et al. :cite:`Haering-etal:2020` and the observation of +discussed in Haering et al. :cite:`Haering-etal:2020` and the observation of “modeled-stress depletion” in other hybrid approaches, such as DES, a mechanism for inducing resolved turbulent fluctuations at proper energy levels and timescales to match your reduction of the modeled @@ -969,14 +994,14 @@
When using AMS with SST as the mean (RANS) contribution to model the Atmospheric Boundary Layer with the Coriolis effect, SST should include a mixing length limiter. The mixing length limiter is described in SST Mixing Length Limiter. For consistency, when using the limiter the RANS time scale, \(T_{RANS}^*\), should depend on the mixing length rather than \(\omega\) to account for the effect of the limiter. The time scale becomes
A fully implicit CVFEM (only) linear elastic equation is supported in the code base. This equation is either used for true solid stress prediction or for smoothing the mesh due to boundary mesh motion (either @@ -1017,7 +1042,7 @@
The code base supports three notions of moving mesh: 1) linear elastic equation system that computes the stress of a solid 2) solid body rotation mesh motion and 3) mesh deformation via an external @@ -1062,7 +1087,7 @@
The spatial variation of the radiative intensity corresponding to a given direction and at a given wavelength within a radiatively participating material, \(I(s)\), is governed by the Boltzmann @@ -1118,11 +1143,11 @@
where \(\theta_{zn}\) and \(\theta_{az}\) are the zenith and azimuthal angles respectively as shown in Figure 2.1.
-RANS and DES simulations using \(k-\omega\) SST or SST-DES equations requires the specification of a wall distance for computing various turbulence parameters. For static mesh @@ -1156,7 +1181,7 @@