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hyStrath
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Issues
A
applications\solvers\compressible\hy2Foam\eqns\evEqnViscous_SingleTv.H
0 2 -
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src\lagrangian\molecularDynamics\polyCloud\measurements\derived\otherFields\polyBindingEnergyRadial\polyBindingEnergyRadial.H
0 2 3
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src\lagrangian\dsmc\coordinateSystem\basic\dsmcCoordinateSystem.H
0 2 5
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src\lagrangian\molecularDynamics\polyCloud\measurements\derived\otherFields\polyDensityMOB2DRadialCOM\polyDensityMOB2DRadialCOM.H
0 2 3
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src\functionObjects\lagrangian\cloudInfo\cloudInfo.H
0 2 3
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src\lagrangian\molecularDynamics\polyCloud\measurements\derived\otherFields\polyDensityRadialNew\polyDensityRadialNew.H
0 2 3
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src\lagrangian\dsmc\coordinateSystem\derived\Cartesian\dsmcCartesian.C
5 2 -
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src\lagrangian\molecularDynamics\polyCloud\measurements\derived\otherFields\polyForceTwoMolecules\polyForceTwoMolecules.H
0 2 3
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applications\utilities\preProcessing\mapFields\MapVolFields.H
2 2 -
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src\lagrangian\molecularDynamics\polyCloud\measurements\derived\otherFields\polyPDB\polyPDB.C
81 3 1
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src\lagrangian\molecularDynamics\polyCloud\measurements\derived\otherFields\polyMoleculePotentialEnergy\polyMoleculePotentialEnergy.H
0 2 3
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src\lagrangian\molecularDynamics\polyCloud\measurements\derived\otherFields\polyFrictionForce\polyFrictionForce.H
0 2 3
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src\lagrangian\dsmc\coordinateSystem\derived\Cartesian\dsmcCartesianI.H
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applications\solvers\compressible\hy2Foam\BCs\mixedFixedValueSlip\mixedFixedValueSlipFvPatchFields.H
0 2 -
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applications\solvers\compressible\hy2Foam\eqns\BEqn.H
0 1 3
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applications\solvers\discreteMethods\molecularDynamics\mdEquilibrationFoam\mdEquilibrationFoam.C
3 2 -
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applications\utilities\parallelProcessing\decomposePar\domainDecomposition.C
38 2 1
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src\TurbulenceModels\compressible\turbulentFluidThermoModels\derivedFvPatchFields\outletMappedUniformInletHeatAddition\outletMappedUniformInletHeatAdditionFvPatchField.H
3 2 1
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src\lagrangian\dsmc\boundaries\derived\generalBoundaries\dsmcWangPressureInlet\dsmcWangPressureInlet.C
29 3 -
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src\lagrangian\molecularDynamics\molecule\mdTools\createAutoCorrelationFunctions.H
0 2 -