  Foam | |
  fvsc | |
   fvscStencil | This is a method for calculation the differential operators without tangential derivatives. They are further used in the calculation of the QGD terms |
| GaussVolPointBase | |
| GaussVolPointBase1D | |
| GaussVolPointBase2D | |
| GaussVolPointBase3D | |
| GaussVolPoint | |
| GaussVolPoint1D | This is a method for approximating derivatives of tangents to a face (1D case). They are further used in the calculation of the QGD terms |
| GaussVolPoint2D | This is a method for approximating derivatives of tangents to a face (2D case). They are further used in the calculation of the QGD terms |
| GaussVolPoint3D | This is a method for approximating derivatives of tangents to a face (3D case). They are further used in the calculation of the QGD terms |
| GaussVolPointBase | This is a method for approximating derivatives of tangents to a face. They are further used in the calculation of the QGD terms |
| GaussVolPointBase1D | |
| GaussVolPointBase2D | |
| GaussVolPointBase3D | |
 GaussVolPointStencil | Methods calculation of differential operators without tangential derivatives |
| leastSquaresBase | |
| leastSquares | |
| extendedFaceStencilCalculateWeights | Base methods for calculating weights |
| extendedFaceStencilFindNeighbours | Base methods for finding neighbours |
| extendedFaceStencilScalarGrad | |
| leastSquaresBase | Base methods for calculating weights and finding neighbours |
| leastSquaresStencil | Realisation least squares method for calculationg of differential operators |
| leastSquaresOpt | |
| extendedFaceStencilFormVfValues | Function for filling of array which contain which will contain the cells necessary for use by several processors. Source file extendedFaceStencilScalarDer.C extendedFaceStencilScalarGradOpt.C leastSquaresStencilOpt.C |
| extendedFaceStencilScalarDer | Methods for optimal calculating of directional derivative. With parallel realisation |
| extendedFaceStencilScalarGradOpt | Methods for optimal calculating of directional derivative. With parallel realisation |
| leastSquaresStencilOpt | Methods for optimal calculating of directional derivative. With parallel realisation |
| reduced | |
| reducedFaceNormalStencil | Methods calculating of differential operators without tangential direvatives |
| qgd | |
| constScPrModel1 | Class describing QGD model coefficients using constant values for Sc^{QGD}, Pr^{QGD} and specified field: |
| constScPrModel1n | Class describing QGD model coefficients using constant values for Sc^{QGD}, Pr^{QGD} and specified field: |
| constScPrModel2 | Class describing QGD model coefficients using constant values for Sc^{QGD}, Pr^{QGD} and specified field: |
| constTau | Class for case constant and uniform distribution |
| H2bynuQHD | Class for one of possible ways of tau calculating |
| HbyUQHD | Class for one of possible ways of $$ calculating. in this case $$ parameter is calculating by |
| QGDCoeffs | Base class for all classes describing QGD model coefficients. Provides interfaces for accessing QGD/QHD models coefficients ^{QGD}, ^{QGD}, ^{QGD}, ^{QGD}, h^{QGD} |
| T0byGr | Class for to calculate $$ as inverse proportional of Grashoff number. in this case $$ parameter is calculated by |
| varScModel5 | Class describing QGD model coefficients using dynamic values for Sc^{QGD}, Pr^{QGD} and specified field: |
| varScModel6 | Class describing QGD model coefficients using dynamic values for Sc^{QGD}, Pr^{QGD} and specified field: |
| varScModel7 | Class describing QGD model coefficients using dynamic values for Sc^{QGD}, Pr^{QGD} and specified field: |
| twoPhaseConstTau | |
| psiQGDThermo | Possible thermo properties for thermo model |
| cosVelocityFvPatchVectorField | This boundary condition sets the pressure gradient to the provided value such that the flux on the boundary is that specified by the velocity boundary condition |
| qgdFluxFvPatchScalarField | This boundary condition sets the pressure gradient to the provided value such that the flux on the boundary is that specified by the velocity boundary condition |
| qhdFluxFvPatchScalarField | This boundary condition sets the pressure gradient to the provided value such that the flux on the boundary is that specified by the velocity boundary condition |
| powerLawTransport | Constant properties Transport package. Templated into a given thermodynamics package (needed for thermal conductivity) |
| psiQGDReactionThermo | Foam::psiQGDReactionThermo |
| hePsiQGDThermo | Energy for a perfect gas mixture with QGD equations |
| psiQGDThermo | Class describing thermophysical properties of perfect gas with motion governed by Quasi- Gas dynamics equations |
| QGDThermo | Abstract base class for classes implementing thermophysical properties of gases and fluids governed by regularized equations (QGD & QHD) |
| heRhoQGDThermo | |
| rhoQGDThermo | Basic thermodynamic properties based on density |
| mQhdFluxFvPatchScalarField | This boundary condition sets the pressure gradient to the provided value such that the flux on the boundary is that specified by the velocity boundary condition |
| qInterfaceProperties | Contains the interface properties |
| constTwoPhaseProperties | |
| twoPhaseIcoQGDThermo | Thermodynamics and mechanics class for incompressible two-phase mixture of immiscible components |
| fvsc | Methods calculating of differential operators |
| heRhoThermo | Energy for a mixture based on density |
| twoPhaseConstTau | Class for one of possible ways of tau calculating |
Generated by
1.8.5
