Commit Graph

434 Commits

Author SHA1 Message Date
728c564246 Minor reformatting 2016-06-12 21:12:13 +01:00
5d7edbc620 Descriptions of solvers corrected and made more consistent and more user-friendly 2016-06-09 18:59:40 +01:00
706ec804fd Added forward declaration of friend functions 2016-05-30 13:21:29 +01:00
758dfc2c1f Standardized the naming of functions which control the writing of fields etc.
to have the prefix 'write' rather than 'output'

So outputTime() -> writeTime()

but 'outputTime()' is still supported for backward-compatibility.

Also removed the redundant secondary-writing functionality from Time
which has been superseded by the 'writeRegisteredObject' functionObject.
2016-05-12 17:38:01 +01:00
4c8556709a applications/solvers: Moved createMRF.H into createField.H
to ensure MRF functionality is available for the -postProcess option
2016-05-09 16:06:12 +01:00
15545786b4 applications/solvers: Added -postProcess option
See also commit 30e2f912e5
2016-05-09 14:08:15 +01:00
4cadaeb3cc applications/solvers/multiphase: Added -postProcess option
See also commit 30e2f912e5
2016-05-08 20:57:08 +01:00
ed3af8dfbf interPhaseChangeFoam, multiphaseInterFoam, potentialFreeSurfaceFoam: Added -postProcess option
See also commit 30e2f912e5
2016-05-08 17:23:36 +01:00
51281bdf8e interFoam: Added -postProcess option
See also commit 30e2f912e5
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1301
2016-05-08 14:32:23 +01:00
92c4c12a08 Multiphase solvers: Update p_rgh following density changes 2016-05-03 15:51:15 +01:00
0f1921787e reactingTwoPhaseEulerFoam: Update p_rgh following density changes
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=2073
2016-05-03 14:53:11 +01:00
bc2fd6c347 applications/solvers: include readTimeControls.H in the time-loop rather than createTimeControls.H
Patch contributed by Bruno Santos
Resolved bug-report http://www.openfoam.org/mantisbt/view.php?id=2079
2016-05-01 11:06:21 +01:00
4da46e7cd9 Updated headers 2016-04-30 21:53:19 +01:00
fe43b80536 GeometricField: Renamed internalField() -> primitiveField() and dimensionedInternalField() -> internalField()
These new names are more consistent and logical because:

primitiveField():
primitiveFieldRef():
    Provides low-level access to the Field<Type> (primitive field)
    without dimension or mesh-consistency checking.  This should only be
    used in the low-level functions where dimensional consistency is
    ensured by careful programming and computational efficiency is
    paramount.

internalField():
internalFieldRef():
    Provides access to the DimensionedField<Type, GeoMesh> of values on
    the internal mesh-type for which the GeometricField is defined and
    supports dimension and checking and mesh-consistency checking.
2016-04-30 21:40:09 +01:00
68fb9a2bf9 GeometricField::dimensionedInteralFieldRef() -> GeometricField::ref()
In order to simplify expressions involving dimensioned internal field it
is preferable to use a simpler access convention.  Given that
GeometricField is derived from DimensionedField it is simply a matter of
de-referencing this underlying type unlike the boundary field which is
peripheral information.  For consistency with the new convention in
"tmp"  "dimensionedInteralFieldRef()" has been renamed "ref()".
2016-04-30 18:43:51 +01:00
e1e996746b GeometricField::internalField() -> GeometricField::internalFieldRef()
Non-const access to the internal field now obtained from a specifically
named access function consistent with the new names for non-canst access
to the boundary field boundaryFieldRef() and dimensioned internal field
dimensionedInternalFieldRef().

See also commit a4e2afa4b3
2016-04-30 14:25:21 +01:00
75ea76187b GeometricField::GeometricBoundaryField -> GeometricField::Boundary
When the GeometricBoundaryField template class was originally written it
was a separate class in the Foam namespace rather than a sub-class of
GeometricField as it is now.  Without loss of clarity and simplifying
code which access the boundary field of GeometricFields it is better
that GeometricBoundaryField be renamed Boundary for consistency with the
new naming convention for the type of the dimensioned internal field:
Internal, see commit a25a449c9e

This is a very simple text substitution change which can be applied to
any code which compiles with the OpenFOAM-dev libraries.
2016-04-28 07:22:02 +01:00
a25a449c9e GeometricField: Rationalized and simplified access to the dimensioned internal field
Given that the type of the dimensioned internal field is encapsulated in
the GeometricField class the name need not include "Field"; the type
name is "Internal" so

volScalarField::DimensionedInternalField -> volScalarField::Internal

In addition to the ".dimensionedInternalField()" access function the
simpler "()" de-reference operator is also provided to greatly simplify
FV equation source term expressions which need not evaluate boundary
conditions.  To demonstrate this kEpsilon.C has been updated to use
dimensioned internal field expressions in the k and epsilon equation
source terms.
2016-04-27 21:32:45 +01:00
97f473ff0f GeometricField::dimensionedInternalField() -> GeometricField::dimensionedInternalFieldRef()
See also commit a4e2afa4b3
2016-04-26 16:29:43 +01:00
a4e2afa4b3 Completed boundaryField() -> boundaryFieldRef()
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1938

Because C++ does not support overloading based on the return-type there
is a problem defining both const and non-const member functions which
are resolved based on the const-ness of the object for which they are
called rather than the intent of the programmer declared via the
const-ness of the returned type.  The issue for the "boundaryField()"
member function is that the non-const version increments the
event-counter and checks the state of the stored old-time fields in case
the returned value is altered whereas the const version has no
side-effects and simply returns the reference.  If the the non-const
function is called within the patch-loop the event-counter may overflow.
To resolve this it in necessary to avoid calling the non-const form of
"boundaryField()" if the results is not altered and cache the reference
outside the patch-loop when mutation of the patch fields is needed.

The most straight forward way of resolving this problem is to name the
const and non-const forms of the member functions differently e.g. the
non-const form could be named:

    mutableBoundaryField()
    mutBoundaryField()
    nonConstBoundaryField()
    boundaryFieldRef()

Given that in C++ a reference is non-const unless specified as const:
"T&" vs "const T&" the logical convention would be

    boundaryFieldRef()
    boundaryFieldConstRef()

and given that the const form which is more commonly used is it could
simply be named "boundaryField()" then the logical convention is

    GeometricBoundaryField& boundaryFieldRef();

    inline const GeometricBoundaryField& boundaryField() const;

This is also consistent with the new "tmp" class for which non-const
access to the stored object is obtained using the ".ref()" member function.

This new convention for non-const access to the components of
GeometricField will be applied to "dimensionedInternalField()" and "internalField()" in the
future, i.e. "dimensionedInternalFieldRef()" and "internalFieldRef()".
2016-04-25 16:16:05 +01:00
8c4f6b8fcb Standardized cell, patch and face loop index names 2016-04-25 10:28:32 +01:00
6a27f7af46 boundaryField() -> boundaryFieldRef() 2016-04-24 22:07:37 +01:00
6a9101990e JohnsonJacksonSchaefferFrictionalStress: Updated I2D expression 2016-04-22 15:13:45 +01:00
6edac8f9ca reactingTwoPhaseEulerFoam: Corrected kineticTheory frictional stress at walls
Patch contributed by Juho Peltola, VTT

The new JohnsonJacksonSchaefferFrictionalStress model is included and
the LBend tutorial case to demonstrate the need for the changes to the
frictional stress models.

Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=2058
2016-04-22 14:25:58 +01:00
287603474a vector::zero -> Zero 2016-04-16 18:34:41 +01:00
fda9aadb3a Specialized dotInterpolate for the efficient calculation of flux fields
e.g. (fvc::interpolate(HbyA) & mesh.Sf()) -> fvc::flux(HbyA)

This removes the need to create an intermediate face-vector field when
computing fluxes which is more efficient, reduces the peak storage and
improved cache coherency in addition to providing a simpler and cleaner
API.
2016-04-06 20:20:53 +01:00
94e9b05edd applications/.*/Allwmake: Updated to support "stop on 1st error"
Patch contributed by Bruno Santos
Resolved bug-report http://www.openfoam.org/mantisbt/view.php?id=2042
2016-04-04 09:03:40 +01:00
fa8929df6d Use Zero rather than pTraits<Type>::zero unless a static typed '0' is required 2016-03-22 17:46:52 +00:00
44c73bfbe1 Made all template declarations consistent using 'class' rather than 'typename' 2016-03-22 15:02:55 +00:00
926c29e95a reactingEulerFoam: Moved fluid.correctThermo() into energy corrector loop
to update the interfacial temperature.
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=2029
2016-03-17 08:05:08 +00:00
c26d5ee31a driftFluxFoam/relativeVelocityModels/general/general:: Corrected construction of residualAlpha 2016-03-15 20:33:06 +00:00
0ef2082dad JohnsonJacksonParticle*FvPatchScalarField.C: Corrected null-construction initialization
Resolves bug-report http://openfoam.org/mantisbt/view.php?id=2022
2016-03-08 14:13:05 +00:00
1b9d8d2954 reactingTwoPhaseEulerFoam: Corrected mass exchange terms in the face-momentum equation
Thanks to Juho Peltola for the patch
2016-03-06 19:02:43 +00:00
c544bec896 Removed duplicate, inconsistent and spurious comments in .C files 2016-02-29 18:33:54 +00:00
99c000fc94 Rationalized the indentation of C-preprocessor directives 2016-02-29 15:42:03 +00:00
7859083246 OpenFOAM: Updated all libraries, solvers and utilities to use the new const-safe tmp
The deprecated non-const tmp functionality is now on the compiler switch
NON_CONST_TMP which can be enabled by adding -DNON_CONST_TMP to EXE_INC
in the Make/options file.  However, it is recommended to upgrade all
code to the new safer tmp by using the '.ref()' member function rather
than the non-const '()' dereference operator when non-const access to
the temporary object is required.

Please report any problems on Mantis.

Henry G. Weller
CFD Direct.
2016-02-26 17:31:28 +00:00
feb3fc43d0 reactingTwoPhaseEulerFoam/Make/options: Removed temporary debug option 2016-02-24 14:05:20 +00:00
3a56ebf33d tmp: Improved reference count checks to provide better error diagnostics
in case of tmp misuse.

Simplified tmp reuse pattern in field algebra to use tmp copy and
assignment rather than the complex delayed call to 'ptr()'.

Removed support for unused non-const 'REF' storage of non-tmp objects due to C++
limitation in constructor overloading: if both tmp(T&) and tmp(const T&)
constructors are provided resolution is ambiguous.

The turbulence libraries have been upgraded and '-DCONST_TMP' option
specified in the 'options' file to switch to the new 'tmp' behavior.
2016-02-24 12:47:36 +00:00
4758c2ac86 tmp: Updated to store and preserve the const-ness of the reference to a constant object
This change requires that the de-reference operator '()' returns a
const-reference to the object stored irrespective of the const-ness of
object stored and the new member function 'ref()' is provided to return
an non-const reference to stored object which throws a fatal error if the
stored object is const.

In order to smooth the transition to this new safer 'tmp' the now
deprecated and unsafe non-const de-reference operator '()' is still
provided by default but may be switched-off with the compilation switch
'CONST_TMP'.

The main OpenFOAM library has already been upgraded and '-DCONST_TMP'
option specified in the 'options' file to switch to the new 'tmp'
behavior.  The rest of OpenFOAM-dev will be upgraded over the following
few weeks.

Henry G. Weller
CFD Direct
2016-02-22 16:23:21 +00:00
7d192447f0 Boundary conditions: Added extrapolatedCalculatedFvPatchField
To be used instead of zeroGradientFvPatchField for temporary fields for
which zero-gradient extrapolation is use to evaluate the boundary field
but avoiding fields derived from temporary field using field algebra
inheriting the zeroGradient boundary condition by the reuse of the
temporary field storage.

zeroGradientFvPatchField should not be used as the default patch field
for any temporary fields and should be avoided for non-temporary fields
except where it is clearly appropriate;
extrapolatedCalculatedFvPatchField and calculatedFvPatchField are
generally more suitable defaults depending on the manner in which the
boundary values are specified or evaluated.

The entire OpenFOAM-dev code-base has been updated following the above
recommendations.

Henry G. Weller
CFD Direct
2016-02-20 22:44:37 +00:00
5e4822b974 kineticTheoryModel: Corrected handling of the SuSp term in the Theta equation
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=2002
2016-02-19 13:26:41 +00:00
19497ce518 interFoam, interMixingFoam, interPhaseChangeFoam: construct rho with calculated BCs
Avoids problems with inherited complex BCs for which the controlling
fields and parameters are not initialized.
2016-02-18 21:26:25 +00:00
fa0656c358 scripts: Reformat with consistent section separators 2016-02-15 18:30:24 +00:00
acaf72b4b4 Solvers: Added support for extrapolated pressure boundary conditions
The boundary conditions of HbyA are now constrained by the new "constrainHbyA"
function which applies the velocity boundary values for patches for which the
velocity cannot be modified by assignment and pressure extrapolation is
not specified via the new
"fixedFluxExtrapolatedPressureFvPatchScalarField".

The new function "constrainPressure" sets the pressure gradient
appropriately for "fixedFluxPressureFvPatchScalarField" and
"fixedFluxExtrapolatedPressureFvPatchScalarField" boundary conditions to
ensure the evaluated flux corresponds to the known velocity values at
the boundary.

The "fixedFluxPressureFvPatchScalarField" boundary condition operates
exactly as before, ensuring the correct flux at fixed-flux boundaries by
compensating for the body forces (gravity in particular) with the
pressure gradient.

The new "fixedFluxExtrapolatedPressureFvPatchScalarField" boundary
condition may be used for cases with or without body-forces to set the
pressure gradient to compensate not only for the body-force but also the
extrapolated "HbyA" which provides a second-order boundary condition for
pressure.  This is useful for a range a problems including impinging
flow, extrapolated inlet conditions with body-forces or for highly
viscous flows, pressure-induced separation etc.  To test this boundary
condition at walls in the motorBike tutorial case set

    lowerWall
    {
        type            fixedFluxExtrapolatedPressure;
    }

    motorBikeGroup
    {
        type            fixedFluxExtrapolatedPressure;
    }

Currently the new extrapolated pressure boundary condition is supported
for all incompressible and sub-sonic compressible solvers except those
providing implicit and tensorial porosity support.  The approach will be
extended to cover these solvers and options in the future.

Note: the extrapolated pressure boundary condition is experimental and
requires further testing to assess the range of applicability,
stability, accuracy etc.

Henry G. Weller
CFD Direct Ltd.
2016-02-13 17:48:26 +00:00
626580f524 driftFluxFoam: Set Udm BCs to type calculated 2016-02-11 08:48:15 +00:00
3e48c61eb3 reactingEulerFoam/interfacialModels/wallLubricationModels: Apply zero-gradient condition at walls 2016-01-19 15:26:42 +00:00
7f67b3e46e reactingEulerFoam,twoPhaseEulerFoam: Corrected pressure equations for transonic operation
Resolves bug-report http://openfoam.org/mantisbt/view.php?id=1971
2016-01-17 11:02:21 +00:00
a56ab5f863 Consistently indent continuation backslashes in macro definitions 2016-01-11 13:00:56 +00:00
94c05a1e6c Update code to use the simpler C++11 template syntax removing spaces between closing ">"s 2016-01-10 22:41:16 +00:00
6b3af46cdf reactingEulerFoam/interfacialModels/dragModels/TomiyamaKataokaZunSakaguchi: New drag model
Drag model for gas-liquid system of Tomiyama et al.

Reference:
    "Drag coefficients of single bubbles under normal and microgravity
     conditions"
    Tomiyama, A., Kataoka, I., Zun, I., Sakaguchi, T.
    JSME International Series B, Fluids and Thermal Engineering,
    Vol. 41, 1998, pp. 472-479

Provided by Alberto Passalacq
2015-12-09 16:51:46 +00:00