mirror of
https://develop.openfoam.com/Development/openfoam.git
synced 2025-11-28 03:28:01 +00:00
STYLE: some general spelling fixes
This commit is contained in:
@ -35,7 +35,7 @@ Description
|
||||
|
||||
Combusting RANS code using the b-Xi two-equation model.
|
||||
Xi may be obtained by either the solution of the Xi transport
|
||||
equation or from an algebraic exression. Both approaches are
|
||||
equation or from an algebraic expression. Both approaches are
|
||||
based on Gulder's flame speed correlation which has been shown
|
||||
to be appropriate by comparison with the results from the
|
||||
spectral model.
|
||||
@ -66,7 +66,7 @@ Description
|
||||
CR | Drag tensor (1/m)
|
||||
CT | Turbulence generation parameter (1/m)
|
||||
Nv | Number of obstacles in cell per unit volume (m^-2)
|
||||
nsv | Tensor whose diagonal indicates the number to substract from
|
||||
nsv | Tensor whose diagonal indicates the number to subtract from
|
||||
| Nv to get the number of obstacles crossing the flow in each
|
||||
| direction.
|
||||
\endplaintable
|
||||
|
||||
@ -32,7 +32,7 @@ Description
|
||||
|
||||
Combusting RANS code using the b-Xi two-equation model.
|
||||
Xi may be obtained by either the solution of the Xi transport
|
||||
equation or from an algebraic exression. Both approaches are
|
||||
equation or from an algebraic expression. Both approaches are
|
||||
based on Gulder's flame speed correlation which has been shown
|
||||
to be appropriate by comparison with the results from the
|
||||
spectral model.
|
||||
|
||||
@ -28,7 +28,7 @@ Global
|
||||
|
||||
Description
|
||||
Reset the timestep to maintain a constant maximum courant Number.
|
||||
Reduction of time-step is imediate but increase is damped to avoid
|
||||
Reduction of time-step is immediate but increase is damped to avoid
|
||||
unstable oscillations.
|
||||
|
||||
\*---------------------------------------------------------------------------*/
|
||||
|
||||
@ -36,7 +36,7 @@ Description
|
||||
|
||||
Combusting RANS code using the b-Xi two-equation model.
|
||||
Xi may be obtained by either the solution of the Xi transport
|
||||
equation or from an algebraic exression. Both approaches are
|
||||
equation or from an algebraic expression. Both approaches are
|
||||
based on Gulder's flame speed correlation which has been shown
|
||||
to be appropriate by comparison with the results from the
|
||||
spectral model.
|
||||
|
||||
@ -31,7 +31,7 @@ Description
|
||||
|
||||
Combusting RANS code using the b-Xi two-equation model.
|
||||
Xi may be obtained by either the solution of the Xi transport
|
||||
equation or from an algebraic exression. Both approaches are
|
||||
equation or from an algebraic expression. Both approaches are
|
||||
based on Gulder's flame speed correlation which has been shown
|
||||
to be appropriate by comparison with the results from the
|
||||
spectral model.
|
||||
|
||||
@ -35,7 +35,7 @@ Description
|
||||
|
||||
Combusting RANS code using the b-Xi two-equation model.
|
||||
Xi may be obtained by either the solution of the Xi transport
|
||||
equation or from an algebraic exression. Both approaches are
|
||||
equation or from an algebraic expression. Both approaches are
|
||||
based on Gulder's flame speed correlation which has been shown
|
||||
to be appropriate by comparison with the results from the
|
||||
spectral model.
|
||||
|
||||
@ -119,7 +119,7 @@ int main(int argc, char *argv[])
|
||||
alphac = max(1.0 - kinematicCloud.theta(), alphacMin);
|
||||
alphac.correctBoundaryConditions();
|
||||
|
||||
Info<< "Continous phase-1 volume fraction = "
|
||||
Info<< "Continuous phase-1 volume fraction = "
|
||||
<< alphac.weightedAverage(mesh.Vsc()).value()
|
||||
<< " Min(alphac) = " << min(alphac).value()
|
||||
<< " Max(alphac) = " << max(alphac).value()
|
||||
|
||||
@ -28,7 +28,7 @@ Global
|
||||
|
||||
Description
|
||||
Reset the timestep to maintain a constant maximum courant Number.
|
||||
Reduction of time-step is imediate but increase is damped to avoid
|
||||
Reduction of time-step is immediate but increase is damped to avoid
|
||||
unstable oscillations.
|
||||
|
||||
\*---------------------------------------------------------------------------*/
|
||||
|
||||
@ -28,7 +28,7 @@ Class
|
||||
|
||||
Description
|
||||
Contact-angle boundary condition for multi-phase interface-capturing
|
||||
simulations. Used in conjuction with multiphaseMixture.
|
||||
simulations. Used in conjunction with multiphaseMixture.
|
||||
|
||||
SourceFiles
|
||||
alphaContactAngleFvPatchScalarField.C
|
||||
|
||||
@ -143,7 +143,7 @@ public:
|
||||
const volScalarField& Tf
|
||||
) const;
|
||||
|
||||
//- Reference mass fraction for specied based models
|
||||
//- Reference mass fraction for species based models
|
||||
virtual tmp<volScalarField> Yf
|
||||
(
|
||||
const word& speciesName,
|
||||
|
||||
@ -27,7 +27,7 @@ Class
|
||||
Foam::meltingEvaporationModels::Lee
|
||||
|
||||
Description
|
||||
Mass tranfer Lee model. Simple model driven by field value difference as:
|
||||
Mass transfer Lee model. Simple model driven by field value difference as:
|
||||
|
||||
\f[
|
||||
\dot{m} = C \rho \alpha (T - T_{activate})/T_{activate}
|
||||
|
||||
@ -27,7 +27,7 @@ Class
|
||||
Foam::interfaceCompositionModel
|
||||
|
||||
Description
|
||||
Generic base class for interface models. Mass transer models are
|
||||
Generic base class for interface models. Mass transfer models are
|
||||
interface models between two thermos.
|
||||
Abstract class for mass transfer functions
|
||||
|
||||
|
||||
@ -40,7 +40,7 @@ Description
|
||||
Flux | mass flux rate [kg/s/m2]
|
||||
M | molecular weight
|
||||
T_{activate} | saturation temperature
|
||||
C | accomodation coefficient
|
||||
C | accommodation coefficient
|
||||
R | universal gas constant
|
||||
p_{sat} | saturation pressure
|
||||
p | vapor partial pressure
|
||||
@ -70,7 +70,7 @@ Description
|
||||
(T - T_{activate})
|
||||
\f]
|
||||
|
||||
This assumes liquid and vapour are in equilibrium, then the accomodation
|
||||
This assumes liquid and vapour are in equilibrium, then the accommodation
|
||||
coefficient are equivalent for the interface. This relation is known as the
|
||||
Hertz-Knudsen-Schrage.
|
||||
|
||||
@ -145,7 +145,7 @@ class kineticGasEvaporation
|
||||
//- Activation temperature
|
||||
const dimensionedScalar Tactivate_;
|
||||
|
||||
//- Molar weight of the vapour in the continous phase
|
||||
//- Molar weight of the vapour in the continuous phase
|
||||
dimensionedScalar Mv_;
|
||||
|
||||
//- Interface area
|
||||
|
||||
@ -267,7 +267,7 @@ public:
|
||||
|
||||
// Energy related thermo functionaliy functions
|
||||
|
||||
//- Return access to the inernal energy field [J/Kg]
|
||||
//- Return access to the internal energy field [J/Kg]
|
||||
// \note this mixture thermo is prepared to work with T
|
||||
virtual volScalarField& he()
|
||||
{
|
||||
@ -275,7 +275,7 @@ public:
|
||||
return const_cast<volScalarField&>(volScalarField::null());
|
||||
}
|
||||
|
||||
//- Return access to the inernal energy field [J/Kg]
|
||||
//- Return access to the internal energy field [J/Kg]
|
||||
// \note this mixture thermo is prepared to work with T
|
||||
virtual const volScalarField& he() const
|
||||
{
|
||||
|
||||
@ -28,7 +28,7 @@ Class
|
||||
|
||||
Description
|
||||
Contact-angle boundary condition for multi-phase interface-capturing
|
||||
simulations. Used in conjuction with multiphaseSystem.
|
||||
simulations. Used in conjunction with multiphaseSystem.
|
||||
|
||||
SourceFiles
|
||||
alphaContactAngleFvPatchScalarField.C
|
||||
|
||||
@ -31,7 +31,7 @@ Description
|
||||
Incompressible multi-phase mixture with built in solution for the
|
||||
phase fractions with interface compression for interface-capturing.
|
||||
|
||||
Derived from transportModel so that it can be unsed in conjunction with
|
||||
Derived from transportModel so that it can be unused in conjunction with
|
||||
the incompressible turbulence models.
|
||||
|
||||
Surface tension and contact-angle is handled for the interface
|
||||
|
||||
@ -28,7 +28,7 @@ Class
|
||||
|
||||
Description
|
||||
Contact-angle boundary condition for multi-phase interface-capturing
|
||||
simulations. Used in conjuction with multiphaseMixture.
|
||||
simulations. Used in conjunction with multiphaseMixture.
|
||||
|
||||
SourceFiles
|
||||
alphaContactAngleFvPatchScalarField.C
|
||||
|
||||
@ -30,7 +30,7 @@ Description
|
||||
Incompressible multi-phase mixture with built in solution for the
|
||||
phase fractions with interface compression for interface-capturing.
|
||||
|
||||
Derived from transportModel so that it can be unsed in conjunction with
|
||||
Derived from transportModel so that it can be unused in conjunction with
|
||||
the incompressible turbulence models.
|
||||
|
||||
Surface tension and contact-angle is handled for the interface
|
||||
|
||||
Reference in New Issue
Block a user