This change means this function is determining the sequence in which
points are plotted topologically. This makes it possible to plot a layer
average along a pipe that goes through many changes of direction.
Previously, the function determined the order by means of a geometric
sort in the plot direction. This only worked when the layers were
perpendicular to one of the coordinate axes.
This is a simple function that provides a convenient way for a user to
call fvc::reconstruct for the purposes of post-processing flux fields;
e.g., to construct a cell velocity from a face flux.
It can be used to generate output during a run by adding the following
settings to a case's controlDict:
functions
{
#includeFunc reconstruct(phi)
}
Or it can be executed as a postProcessing step by calling:
postProcess -func "reconstruct(phi)"
Following the addition of the new moments functionObject, all related
functionality was removed from sizeDistribution.
In its revised version, sizeDistribution allows for different kinds of
weighted region averaging in case of field-dependent representative
particle properties.
A packaged function has also been added to allow for command line solver
post-processing.
For example, the following function object specification returns the
volume-based number density function:
numberDensity
{
type sizeDistribution;
libs ("libmultiphaseEulerFoamFunctionObjects.so");
writeControl writeTime;
populationBalance bubbles;
functionType numberDensity;
coordinateType volume;
setFormat raw;
}
The same can be achieved using a packaged function:
#includeFunc sizeDistribution
(
populationBalance=bubbles,
functionType=numberDensity,
coordinateType=volume,
funcName=numberDensity
)
Or on the command line:
multiphaseEulerFoam -postProcess -func "
sizeDistribution
(
populationBalance=bubbles,
functionType=numberDensity,
coordinateType=volume,
funcName=numberDensity
)"
Patch contributed by Institute of Fluid Dynamics,
Helmholtz-Zentrum Dresden - Rossendorf (HZDR)
This function calculates integral (integer moments) or mean properties
(mean, variance, standard deviation) of a size distribution computed with
multiphaseEulerFoam. It has to be run with multiphaseEulerFoam, either
at run-time or with -postProcess. It will not work with the postProcess
utility.
The following function object specification for example returns the first
moment of the volume-based number density function which is equivalent to
the phase fraction of the particulate phase:
moments
{
type moments;
libs ("libmultiphaseEulerFoamFunctionObjects.so");
executeControl timeStep;
writeControl writeTime;
populationBalance bubbles;
momentType integerMoment;
coordinateType volume;
order 1;
}
The same can be achieved using a packaged function:
#includeFunc moments
(
populationBalance=bubbles,
momentType=integerMoment,
coordinateType=volume,
order=1,
funcName=moments
)
Or on the command line:
multiphaseEulerFoam -postProcess -func "
moments
(
populationBalance=bubbles,
momentType=integerMoment,
coordinateType=volume,
order=1,
funcName=moments
)"
Patch contributed by Institute of Fluid Dynamics,
Helmholtz-Zentrum Dresden - Rossendorf (HZDR)
This function generates plots of fields averaged over the layers in the
mesh. It is a generalised replacement for the postChannel utility, which
has been removed. An example of this function's usage is as follows:
layerAverage1
{
type layerAverage;
libs ("libfieldFunctionObjects.so");
writeControl writeTime;
setFormat raw;
// Patches and/or zones from which layers extrude
patches (bottom);
zones (quarterPlane threeQuartersPlane);
// Spatial component against which to plot
component y;
// Is the geometry symmetric around the centre layer?
symmetric true;
// Fields to average and plot
fields (pMean pPrime2Mean UMean UPrime2Mean k);
}
Sampled sets and streamlines now write all their fields to the same
file. This prevents excessive duplication of the geometry and makes
post-processing tasks more convenient.
"axis" entries are now optional in sampled sets and streamlines. When
omitted, a default entry will be used, which is chosen appropriately for
the coordinate set and the write format. Some combinations are not
supported. For example, a scalar ("x", "y", "z" or "distance") axis
cannot be used to write in the vtk format, as vtk requires 3D locations
with which to associate data. Similarly, a point ("xyz") axis cannot be
used with the gnuplot format, as gnuplot needs a single scalar to
associate with the x-axis.
Streamlines can now write out fields of any type, not just scalars and
vectors, and there is no longer a strict requirement for velocity to be
one of the fields.
Streamlines now output to postProcessing/<functionName>/time/<file> in
the same way as other functions. The additional "sets" subdirectory has
been removed.
The raw set writer now aligns columns correctly.
The handling of segments in coordSet and sampledSet has been
fixed/completed. Segments mean that a coordinate set can represent a
number of contiguous lines, disconnected points, or some combination
thereof. This works in parallel; segments remain contiguous across
processor boundaries. Set writers now only need one write method, as the
previous "writeTracks" functionality is now handled by streamlines
providing the writer with the appropriate segment structure.
Coordinate sets and set writers now have a convenient programmatic
interface. To write a graph of A and B against some coordinate X, in
gnuplot format, we can call the following:
setWriter::New("gnuplot")->write
(
directoryName,
graphName,
coordSet(true, "X", X), // <-- "true" indicates a contiguous
"A", // line, "false" would mean
A, // disconnected points
"B",
B
);
This write function is variadic. It supports any number of
field-name-field pairs, and they can be of any primitive type.
Support for Jplot and Xmgrace formats has been removed. Raw, CSV,
Gnuplot, VTK and Ensight formats are all still available.
The old "graph" functionality has been removed from the code, with the
exception of the randomProcesses library and associated applications
(noise, DNSFoam and boxTurb). The intention is that these should also
eventually be converted to use the setWriters. For now, so that it is
clear that the "graph" functionality is not to be used elsewhere, it has
been moved into a subdirectory of the randomProcesses library.
Description
Evolves a passive scalar transport equation.
- To specify the field name set the \c field entry
- To employ the same numerical schemes as another field set
the \c schemesField entry,
- The \c diffusivity entry can be set to \c none, \c constant, \c viscosity
- A constant diffusivity is specified with the \c D entry,
- If a momentum transport model is available and the \c viscosity
diffusivety option specified an effective diffusivity may be constructed
from the laminar and turbulent viscosities using the diffusivity
coefficients \c alphal and \c alphat:
\verbatim
D = alphal*nu + alphat*nut
\endverbatim
Example:
\verbatim
#includeFunc scalarTransport(T, alphaD=1, alphaDt=1)
\endverbatim
For incompressible flow the passive scalar may optionally be solved with the
MULES limiter and sub-cycling or semi-implicit in order to maintain
boundedness, particularly if a compressive, PLIC or MPLIC convection
scheme is used.
Example:
\verbatim
#includeFunc scalarTransport(tracer, diffusion=none)
with scheme specification:
div(phi,tracer) Gauss interfaceCompression vanLeer 1;
and solver specification:
tracer
{
nCorr 1;
nSubCycles 3;
MULESCorr no;
nLimiterIter 5;
applyPrevCorr yes;
solver smoothSolver;
smoother symGaussSeidel;
tolerance 1e-8;
relTol 0;
diffusion
{
solver smoothSolver;
smoother symGaussSeidel;
tolerance 1e-8;
relTol 0;
}
}
\endverbatim
The surfaceInterpolate function object is now a field expression. This
means it works in the same way as mag, grad, etc... It also now has a
packaged configuration and has been included into the postProcessing
test case.
It can be used in the following ways. On the command line:
postProcess -func "surfaceInterpolate(rho, result=rhof)"
rhoPimpleFoam -postProcess -func "surfaceInterpolate(thermo:rho, result=rhof)"
In the controlDict:
functions
{
#includeFunc surfaceInterpolate(rho, result=rhof)
}
By running:
foamGet surfaceInterpolate
Then editing the resulting system/surfaceInterpolate file and then
running postProcess or adding an #includeFunc entry without arguments.
Packaged function objects can now be deployed equally effectively by
(a) using a locally edited copy of the configuration file, or by
(b) passing parameters as arguments to the global configuration file.
For example, to post-process the pressure field "p" at a single location
"(1 2 3)", the user could first copy the "probes" packaged function
object file to their system directory by calling "foamGet probes". They
could then edit the file to contain the following entries:
points ((1 2 3));
field p;
The function object can then be executed by the postProcess application:
postProcess -func probes
Or it can be called at run-time, by including from within the functions
section of the system/controlDict file:
#includeFunc probes
Alternatively, the field and points parameters could be passed as
arguments either to the postProcess application by calling:
postProcess -func "probes(points=((1 2 3)), p)"
Or by using the #includeFunc directive:
#includeFunc probes(points=((1 2 3)), p)
In both cases, mandatory parameters that must be either edited or
provided as arguments are denoted in the configuration files with
angle-brackets, e.g.:
points (<points>);
Many of the packaged function objects have been split up to make them
more specific to a particular use-case. For example, the "surfaces"
function has been split up into separate functions for each surface
type; "cutPlaneSurface", "isoSurface", and "patchSurface". This
splitting means that the packaged functions now only contain one set of
relevant parameters so, unlike previously, they now work effectively
with their parameters passed as arguments. To ensure correct usage, all
case-dependent parameters are considered mandatory.
For example, the "streamlines" packaged function object has been split
into specific versions; "streamlinesSphere", "streamlinesLine",
"streamlinesPatch" and "streamlinesPoints". The name ending denotes the
seeding method. So, the following command creates ten streamlines with
starting points randomly seeded within a sphere with a specified centre
and radius:
postProcess -func "streamlinesSphere(nPoints=10, centre=(0 0 0), radius=1)"
The equivalent #includeFunc approach would be:
#includeFunc streamlinesSphere(nPoints=10, centre=(0 0 0), radius=1)
When passing parameters as arguments, error messages report accurately
which mandatory parameters are missing and provide instructions to
correct the format of the input. For example, if "postProcess -func
graphUniform" is called, then the code prints the following error message:
--> FOAM FATAL IO ERROR:
Essential value for keyword 'start' not set
Essential value for keyword 'end' not set
Essential value for keyword 'nPoints' not set
Essential value for keyword 'fields' not set
In function entry:
graphUniform
In command:
postProcess -func graphUniform
The function entry should be:
graphUniform(start = <point>, end = <point>, nPoints = <number>, fields = (<fieldNames>))
file: controlDict/functions/graphUniform from line 15 to line 25.
As always, a full list of all packaged function objects can be obtained
by running "postProcess -list", and a description of each function can
be obtained by calling "foamInfo <functionName>". An example case has
been added at "test/postProcessing/channel" which executes almost all
packaged function objects using both postProcess and #includeFunc. This
serves both as an example of syntax and as a unit test for maintenance.
The fieldsExpression function has been generalised to work with a
general operator. Existing functions "add" and "subtract" have been made
to use this system, and two new operations, "multiply" and "divide",
have been added.
The functions can now handle multiple types in both input and output. A
multiply (outer product) operation on two vectors and a scalar will
result in a tensor. If the operation chain is not supported (e.g.,
division by a vector) then a warning will be generated.
In addition, a "uniform" function has been added, which will create a
uniform geometric field of a given type with specified dimensions and
calculated boundary conditions. This is mostly useful for testing
purposes and for conveniently creating simple input fields for the
operation functions described above. The function can be called by
postProcess as follows:
postProcess -func "uniform(fieldType=volScalarField, name=length, dimensions=[m], value=2)"
A number of changes have been made to the surfaceFieldValue and
volFieldValue function objects to improve their usability and
performance, and to extend them so that similar duplicate functionality
elsewhere in OpenFOAM can be removed.
Weighted operations have been removed. Weighting for averages and sums
is now triggered simply by the existence of the "weightField" or
"weightFields" entry. Multiple weight fields are now supported in both
functions.
The distinction between oriented and non-oriented fields has been
removed from surfaceFieldValue. There is now just a single list of
fields which are operated on. Instead of oriented fields, an
"orientedSum" operation has been added, which should be used for
flowRate calculations and other similar operations on fluxes.
Operations minMag and maxMag have been added to both functions, to
calculate the minimum and maximum field magnitudes respectively. The min
and max operations are performed component-wise, as was the case
previously.
In volFieldValue, minMag and maxMag (and min and mag operations when
applied to scalar fields) will report the location, cell and processor
of the maximum or minimum value. There is also a "writeLocation" option
which if set will write this location information into the output file.
The fieldMinMax function has been made obsolete by this change, and has
therefore been removed.
surfaceFieldValue now operates in parallel without accumulating the
entire surface on the master processor for calculation of the operation.
Collecting the entire surface on the master processor is now only done
if the surface itself is to be written out.
Originally the only supported geometry specification were triangulated surfaces,
hence the name of the directory: constant/triSurface, however now that other
surface specifications are supported and provided it is much more logical that
the directory is named accordingly: constant/geometry. All tutorial and
template cases have been updated.
Note that backward compatibility is provided such that if the constant/geometry
directory does not exist but constant/triSurface does then the geometry files
are read from there.
A volumetric flow rate through a tri-surface can now be obtained using
the volumetricFlowRateTriSurface preconfigured function object, using
the following entry in system/controlDict:
fuctions
{
#includeFunc "volumetricFlowRateTriSurface(name=surface.stl)"
}
Where "surface.stl" is a tri-surface file in the constant/triSurface
directory. An example of this has been added to the
incompressible/pimpleFoam/RAS/impeller tutorial case.
Note that when possible, it is preferable to use the flowRatePatch or
flowRateFaceZone functions, as these make direct use of the flux and
therefore report a value that is exactly that computed by the solver.
volumetricFlowRateTriSurface, by contrast, does interpolation of the
velocity field which introduces error.
In addition, a minor fix has been made to the underlying
surfaceFieldValue function object so that it does not need a zone/set
name when values on a searchable surface are requested.
The standard set of Lagrangian clouds are now selectable at run-time.
This means that a solver that supports Lagrangian modelling can now use
any type of cloud (with some restrictions). Previously, solvers were
hard-coded to use specific cloud modelling. In addition, a cloud-list
structure has been added so that solvers may select multiple clouds,
rather than just one.
The new system is controlled as follows:
- If only a single cloud is required, then the settings for the
Lagrangian modelling should be placed in a constant/cloudProperties
file.
- If multiple clouds are required, then a constant/clouds file should be
created containing a list of cloud names defined by the user. Each
named cloud then reads settings from a corresponding
constant/<cloudName>Properties file. Clouds are evolved sequentially
in the order in which they are listed in the constant/clouds file.
- If no clouds are required, then the constant/cloudProperties file and
constant/clouds file should be omitted.
The constant/cloudProperties or constant/<cloudName>Properties files are
the same as previous cloud properties files; e.g.,
constant/kinematicCloudProperties or constant/reactingCloud1Properties,
except that they now also require an additional top-level "type" entry
to select which type of cloud is to be used. The available options for
this entry are:
type cloud; // A basic cloud of solid
// particles. Includes forces,
// patch interaction, injection,
// dispersion and stochastic
// collisions. Same as the cloud
// previously used by
// rhoParticleFoam
// (uncoupledKinematicParticleFoam)
type collidingCloud; // As "cloud" but with resolved
// collision modelling. Same as the
// cloud previously used by DPMFoam
// and particleFoam
// (icoUncoupledKinematicParticleFoam)
type MPPICCloud; // As "cloud" but with MPPIC
// collision modelling. Same as the
// cloud previously used by
// MPPICFoam.
type thermoCloud; // As "cloud" but with
// thermodynamic modelling and heat
// transfer with the carrier phase.
// Same as the limestone cloud
// previously used by
// coalChemistryFoam.
type reactingCloud; // As "thermoCloud" but with phase
// change and mass transfer
// coupling with the carrier
// phase. Same as the cloud
// previously used in fireFoam.
type reactingMultiphaseCloud; // As "reactingCloud" but with
// particles that contain multiple
// phases. Same as the clouds
// previously used in
// reactingParcelFoam and
// simpleReactingParcelFoam and the
// coal cloud used in
// coalChemistryFoam.
type sprayCloud; // As "reactingCloud" but with
// additional spray-specific
// collision and breakup modelling.
// Same as the cloud previously
// used in sprayFoam and
// engineFoam.
The first three clouds are not thermally coupled, so are available in
all Lagrangian solvers. The last four are thermally coupled and require
access to the carrier thermodynamic model, so are only available in
compressible Lagrangian solvers.
This change has reduced the number of solvers necessary to provide the
same functionality; solvers that previously differed only in their
Lagrangian modelling can now be combined. The Lagrangian solvers have
therefore been consolidated with consistent naming as follows.
denseParticleFoam: Replaces DPMFoam and MPPICFoam
reactingParticleFoam: Replaces sprayFoam and coalChemistryFoam
simpleReactingParticleFoam: Replaces simpleReactingParcelFoam
buoyantReactingParticleFoam: Replaces reactingParcelFoam
fireFoam and engineFoam remain, although fireFoam is likely to be merged
into buoyantReactingParticleFoam in the future once the additional
functionality it provides is generalised.
Some additional minor functionality has also been added to certain
solvers:
- denseParticleFoam has a "cloudForceSplit" control which can be set in
system/fvOptions.PIMPLE. This provides three methods for handling the
cloud momentum coupling, each of which have different trade-off-s
regarding numerical artefacts in the velocity field. See
denseParticleFoam.C for more information, and also bug report #3385.
- reactingParticleFoam and buoyantReactingParticleFoam now support
moving mesh in order to permit sharing parts of their implementation
with engineFoam.
Description
Stops the run when the specified clock time in second has been reached
and optionally write results before stopping.
The following actions are supported:
- noWriteNow
- writeNow
- nextWrite (default)
Examples of function object specification:
\verbatim
stop
{
type stopAtClockTime;
libs ("libutilityFunctionObjects.so");
stopTime 10;
action writeNow;
}
\endverbatim
will stop the run at the next write after the file "stop" is created in the
case directory.
Usage
\table
Property | Description | Required | Default value
type | type name: stopAtClockTime | yes |
stopTime | Maximum elapsed time [s] | yes |
action | Action executed | no | nextWrite
\endtable
By default the case stops following the next write but stopping immediately with
or without writing are also options.
The stopAtFile functionObject derived from stopAt stops the run when a file
predefined file is created in the case directory:
Description
Stops the run when the specified file is created in the case directory.
The default name of the trigger file is \c $FOAM_CASE/<name> where \c
<name> is the name of the functionObject entry and the default action is \c
nextWrite.
Currently the following action types are supported:
- noWriteNow
- writeNow
- nextWrite
Examples of function object specification:
\verbatim
stop
{
type stopAtFile;
libs ("libutilityFunctionObjects.so");
}
\endverbatim
will stop the run at the next write after the file "stop" is created in the
case directory.
\verbatim
stop
{
type stopAtFile;
libs ("libutilityFunctionObjects.so");
file "$FOAM_CASE/stop";
action writeNow;
}
\endverbatim
will write the fields and stop the run when the file "stop" is created in
the case directory.
Usage
\table
Property | Description | Required | Default value
type | type name: stopAtFile | yes |
file | Trigger file path name | no | $FOAM_CASE/<name>
action | Action executed | no | nextWrite
\endtable
The new multiphaseEulerFoam is based on reactingMultiphaseEulerFoam with some
improvements and rationalisation to assist maintenance and further development.
The phase system solution has been enhanced to handle two phases more
effectively and all two-phase specific models updated for compatibility so that
multiphaseEulerFoam can also replace reactingTwoPhaseEulerFoam.
When running multiphaseEulerFoam with only two-phases the default behaviour is
to solve for both phase-fractions but optionally a reference phase can be
specified so that only the other phase-fraction is solved, providing better
compatibility with the behaviour of reactingTwoPhaseEulerFoam.
All reactingMultiphaseEulerFoam and reactingTwoPhaseEulerFoam tutorials have
been updated for multiphaseEulerFoam.
Description
This functionObject writes the phase-fraction map field alpha.map with
incremental value ranges for each phase
e.g., with values 0-1 for water, 1-2 for air, 2-3 for oil etc.
Example of function object specification:
\verbatim
phaseMap
{
type phaseMap;
libs ("libreactingEulerFoamFunctionObjects.so");
writeControl writeTime;
}
\endverbatim
Usage
\table
Property | Description | Required | Default value
type | type name: phaseMap | yes |
\endtable
This replaces the alphas functionality previously built-in to
reactingMultiphaseEulerFoam so that the storage, calculation and writing of the
phase map field is now under user control.
providing the shear-stress term in the momentum equation for incompressible and
compressible Newtonian, non-Newtonian and visco-elastic laminar flow as well as
Reynolds averaged and large-eddy simulation of turbulent flow.
The general deviatoric shear-stress term provided by the MomentumTransportModels
library is named divDevTau for compressible flow and divDevSigma (sigma =
tau/rho) for incompressible flow, the spherical part of the shear-stress is
assumed to be either included in the pressure or handled separately. The
corresponding stress function sigma is also provided which in the case of
Reynolds stress closure returns the effective Reynolds stress (including the
laminar contribution) or for other Reynolds averaged or large-eddy turbulence
closures returns the modelled Reynolds stress or sub-grid stress respectively.
For visco-elastic flow the sigma function returns the effective total stress
including the visco-elastic and Newtonian contributions.
For thermal flow the heat-flux generated by thermal diffusion is now handled by
the separate ThermophysicalTransportModels library allowing independent run-time
selection of the heat-flux model.
During the development of the MomentumTransportModels library significant effort
has been put into rationalising the components and supporting libraries,
removing redundant code, updating names to provide a more logical, consistent
and extensible interface and aid further development and maintenance. All
solvers and tutorials have been updated correspondingly and backward
compatibility of the input dictionaries provided.
Henry G. Weller
CFD Direct Ltd.
Rather than specifying the controls per field it is simpler to use a single set
of controls for all the fields in the list and use separate instances of the
fieldAverage functionObject for different control sets:
Example of function object specification setting all the optional parameters:
fieldAverage1
{
type fieldAverage;
libs ("libfieldFunctionObjects.so");
writeControl writeTime;
restartOnRestart false;
restartOnOutput false;
periodicRestart false;
restartPeriod 0.002;
base time;
window 10.0;
windowName w1;
mean yes;
prime2Mean yes;
fields (U p);
}
This allows for a simple specification with the optional prime2Mean entry using
#includeFunc fieldAverage(U, p, prime2Mean = yes)
or if the prime2Mean is not needed just
#includeFunc fieldAverage(U, p)
to support the more convenient #includeFunc specification in both
#includeFunc fieldAverage(U.air, U.water, alpha.air, p)
and
#includeFunc fieldAverage(fields = (U.air, U.water, alpha.air, p))
forms.
The mean, prime2Mean and base now have default values:
{
mean on; // (default = on)
prime2Mean on; // (default = off)
base time; // time or iteration (default = time)
window 200; // optional averaging window
windowName w1; // optional window name (default = "")
}
so for the majority of cases for which these defaults are appropriate the
fieldAverage functionObject can now be specified in the functions entry in
controlDict thus:
functions
{
fieldAverage1
{
#includeEtc "caseDicts/postProcessing/fields/fieldAverage.cfg"
fields
(
U.air
U.water
alpha.air
p
);
}
}
also utilising the new fieldAverage.cfg file.
For cases in which these defaults are not appropriate, e.g. the prime2Mean is
also required the optional entries can be specified within sub-dictionaries for
each field, e.g.
fieldAverage1
{
#includeEtc "caseDicts/postProcessing/fields/fieldAverage.cfg"
fields
(
U
{
prime2Mean yes;
}
p
{
prime2Mean yes;
}
);
}
The total enthalpy is calculated as
Ha = ha + K
where
ha is absolute enthalpy
K is the kinetic energy: 1/2*magSqr(U)
The total enthalpy or a particular phase can be calculated by specifying the
optional "phase" name, e.g.
#includeFunc totalEnthalpy(phase = liquid)
This change formalises the usage of the "log" keyword in function
objects. By default, logging to stdout is activated when running
"postProcess" or "<solver> -postProcess", and deactivated when a
function is being executed as part of a run.
This behaviour can now be overridden in the function object dictionary
when operating in either mode.
e.g. given a vol pressure field p
functions
{
// Interpolate the pressure field to the faces
surfacep
{
type surfaceInterpolate;
libs ("libfieldFunctionObjects.so");
fields ((p surfacep));
writeControl none;
}
// Average the surface pressure field over the centre faceZone
#includeFunc faceZoneAverage(name=centre, surfacep)
.
.
.
}
Both the functionObject call context (the command line for postProcess, and the
controlDict path for run-time post-precessing) and the configuration file
context where the arguments are substituted are now printed in the error
message, e.g.
postProcess -func 'patchAverage(name=inlet, ields=(p U))'
generates the message
--> FOAM FATAL IO ERROR:
Essential value for keyword 'fields' not set in function entry
patchAverage(name=inlet, ields=(p U))
in command line postProcess -func patchAverage(name=inlet, ields=(p U))
Placeholder value is <field_names>
file: /home/dm2/henry/OpenFOAM/OpenFOAM-dev/etc/caseDicts/postProcessing/surfaceFieldValue/patchAverage from line 13 to line 17.
and with the following in controlDict
functions
{
#includeFunc patchAverage(name=inlet, ields=(p U))
}
generates the message
--> FOAM FATAL IO ERROR:
Essential value for keyword 'fields' not set in function entry
patchAverage(name=inlet, ields=(p U))
in file /home/dm2/henry/OpenFOAM/OpenFOAM-dev/tutorials/incompressible/pimpleFoam/RAS/pitzDaily/system/controlDict at line 55
Placeholder value is <field_names>
file: /home/dm2/henry/OpenFOAM/OpenFOAM-dev/etc/caseDicts/postProcessing/surfaceFieldValue/patchAverage from line 13 to line 17.
This is like the scalarTrasport function except that the transported
scalar is confined to a single phase of a multiphase simulation. In
addition to the usual specification for the scalarTransport function
(i.e., a field, schemes and solution parameters), the user needs to
specify the phase-flux or a pressure field which can be used to generate
it.
Example usage for interFoam:
phaseScalarTransport1
{
type phaseScalarTransport;
libs ("libsolverFunctionObjects.so");
field s.water;
p p_rgh;
}
Example usage for reactingTwoPhaseEulerFoam:
phaseScalarTransport1
{
type phaseScalarTransport;
libs ("libsolverFunctionObjects.so");
field s.water;
alphaPhi alphaRhoPhi.water;
rho thermo:rho.water;
}
The function will write out both the per-unit-phase field that is solved
for (s.water in the above examples) and also the mixture-total field
(alphaS.water), which is often more convenient for post-processing.
to rationalise the structure and class names to avoid the need for the confusing
addNamedToRunTimeSelectionTable and use instead use the standard
addToRunTimeSelectionTable to populate the run-time selection table.
