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# PostprocessData Module in phasicFlow
The `PostprocessData` module in phasicFlow provides powerful tools for analyzing particle-based simulations both during runtime (in-simulation) and after simulation completion (post-simulation). This document explains how to configure and use the postprocessing features through the dictionary-based input system.
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- in-simulation: this is postprocessing that is active during simulation. When running a solver, it allows for real-time data analysis and adjustments based on the simulation's current state. See bellow to see how you can activate in-simulation postprocessing.
- post-simulation: this is postprocessing that is done after the simulation is completed. It allows for detailed analysis of the simulation results, including data extraction and visualization based on the results that are stored in time-folders. If you want to use post-simulation, you need to run utitlity `postprocessPhasicFlow` in terminal (in the simulation case setup folder) to run the postprocessing. This utility reads the `postprocessDataDict` file and performs the specified operations on the simulation data.
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## 1. Overview
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Postprocessing in phasicFlow allows you to:
- Extract information about particles in specific regions of the domain
- Calculate statistical properties such as averages and sums of particle attributes
- Track specific particles throughout the simulation
- Apply different weighing methods when calculating statistics
- Perform postprocessing at specific time intervals
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## Table of Contents
- [1. Overview ](#1-overview )
- [2. Setting Up Postprocessing ](#2-setting-up-postprocessing )
- [2.1. Basic Configuration ](#21-basic-configuration )
- [3. Time Control Options ](#3-time-control-options )
- [4. Processing Methods ](#4-processing-methods )
- [5. Region Types ](#5-region-types )
- [6. Processing Operations ](#6-processing-operations )
- [6.1. Available Functions in average ](#61-available-functions-in-average )
- [6.2. About fluctuation2 in average function ](#62-about-fluctuation2-in-average-function )
- [6.3. Derived Functions ](#63-derived-functions )
- [6.4. Available Fields ](#64-available-fields )
- [6.5. Optional Parameters ](#65-optional-parameters )
- [7. Examples ](#7-examples )
- [7.1. Example 1: Probing Individual Particles ](#71-example-1-probing-individual-particles )
- [7.2. Example 2: Processing in a Spherical Region ](#72-example-2-processing-in-a-spherical-region )
- [7.3. Example 3: Processing Along a Line ](#73-example-3-processing-along-a-line )
- [8. Advanced Features ](#8-advanced-features )
- [8.1. Special functions applied on fields ](#81-special-functions-applied-on-fields )
- [8.2. Particle Filtering with includeMask ](#82-particle-filtering-with-includemask )
- [8.3. Implementation Notes ](#83-implementation-notes )
- [9. Mathematical Formulations ](#9-mathematical-formulations )
- [10. A complete dictioanry file (postprocessDataDict) ](#10-a-complete-dictioanry-file-postprocessdatadict )
## 2. Setting Up Postprocessing
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Postprocessing is configured through a dictionary file named `postprocessDataDict` which should be placed in the `settings` directory. Below is a detailed explanation of the configuration options.
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### 2.1. Basic Configuration
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The input dictionary, **settings/postprocessDataDict** , may look like this:
```cpp
// PostprocessData dictionary
// Enable/disable postprocessing during simulation
runTimeActive yes; // Options: yes, no
// Shape type - only needed when doing post-simulation processing
shapeType sphere; // Options depend on the simulation type: sphere, grain, etc.
// Default time control for postprocessing components
defaultTimeControl
{
timeControl timeStep; // Options: timeStep, simulationTime, settings
startTime 0; // Start time for postprocessing
endTime 1000; // End time for postprocessing
executionInterval 150; // How frequently to run postprocessing
}
// List of postprocessing components
components
(
// Component definitions here...
);
```
If you want to activate in-simulaiton postprocessing, you need to add these lines to the `settings/settingsDict` file:
```cpp
libs ("libPostprocessData.so");
auxFunctions postprocessData;
```
This will link the postprocessing library to your simulation, allowing you to use its features. Note that, anytime you want to deactivate the in-simulation postprocessing, you can simply change the `runTimeActive` option to `no` in `postprocessDataDict` file.
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## 3. Time Control Options
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Each postprocessing component can either use the default time control settings or define its own. There are three main options for time control:
| Option | Description | Required Parameters |
|--------|-------------|---------------------|
| `timeStep` | Controls execution based on simulation time steps | `startTime` , `endTime` , `executionInterval` |
| `simulationTime` | Controls execution based on simulation time | `startTime` , `endTime` , `executionInterval` |
| `settings` | Uses parameters from settingsDict file | None (defined elsewhere) |
| `default` | Uses the default time control settings (uses `defaultTimeControl` settings)| None (uses default) |
If no time control is specified, the `default` option is used automatically.
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## 4. Processing Methods
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The postprocessing module provides several methods for processing particle data. They are categorized into two main groups: bulk and individual methods.
- **Bulk Methods**: Operate on all particles that are located in a specified locations/regions (cells, spheres, etc.).
- **Individual Methods**: Operate on specific particles, allowing for targeted particle property extraction.
| Method | Property type | Description | Formula |
|--------|------------------|-------------|---------|
| `arithmetic` | bulk | Simple arithmetic mean/sum with equal weights | Each particle contributes equally |
| `uniformDistribution` | bulk | Each particle contributes inversely proportional to the total number of particles | $w_i = 1/n$ where $n$ is the number of particles |
| `GaussianDistribution` | bulk | Weight contribution based on distance from center with Gaussian falloff | $w_i = \exp(-\|x_i - c\|^2/(2\sigma^2))/\sqrt{2\pi\sigma^2}$ |
| `particleProbe` | individual | Extracts values from specific particles | Direct access to particle properties |
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## 5. Region Types
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Regions define where in the domain the postprocessing operations are applied:
| Region Type | Description | Required Parameters | Compatible with |
|-------------|-------------|---------------------|-----------------|
| `sphere` | A spherical region | `radius` , `center` | bulk |
| `multipleSpheres` | Multiple spherical regions | `centers` , `radii` | bulk |
| `line` | Spheres along a line with specified radius | `p1` , `p2` , `nSpheres` , `radius` | bulk |
| `centerPoints` | Specific particles selected by ID | `ids` | individual |
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## 6. Processing Operations
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Within each processing region of type `bulk` , you can define multiple operations to be performed:
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### 6.1. Available Functions in average
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| Function | Property type | Description | Formula | Required Parameters |
|----------|---------------|-------------|---------|---------------------|
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| `average` | bulk | Weighted average of particle field values | see Equation 1 | `field` , `phi` (optional), `threshold` (optional), `includeMask` (optional), `divideByVolume` (optional), `fluctuation2` (optional) |
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| `sum` | bulk | Weighted sum of particle field values | see Equation 2 | `field` , `phi` (optional),`threshold` (optional), `includeMask` (optional), `divideByVolume` (optional) |
Equation 1:
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$$\text{mean} = \frac{\sum_j w_j \cdot \phi_j \cdot \text{field}_j}{\sum_i w_i \cdot \phi_i}$$
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Equation 2:
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$$\text{sum} = \sum_j w_j \cdot \phi_j \cdot \text{field}_j$$
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where:
- $j$ is the index of the particle in the region that also satisfies the `includeMask`
- $i$ is the index of the particle in the region
- $w_j$ is the weight of particle $j$ based on the selected processing method
- $\phi_j$ is the value of the `phi` field for particle $j$ (default is 1)
- $field_j$ is the value of the specified field for particle $j$
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### 6.2. About fluctuation2 in average function
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Fluctuation2 is an optional parameter that can be used to account for fluctuations in the particle field values with respect to mean value of the field.
It is used in the `average` function to calculate the fluctuation of the field values around the mean. The formula for fluctuation2 is:
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$$\text{fluctuation}^2 = \frac{\sum_j w_j \cdot \phi_j \cdot (\text{field}_j - \text{mean})^2}{\sum_i w_i \cdot \phi_i}$$
where:
- `mean` : is the average value of the field in the region.
- `field` : The field to be processed (e.g., `velocity` , `mass` , etc.)
- `fluctuation2` : Optional parameter to account for fluctuations in the particle field values.
### 6.3. Derived Functions
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In addition to the above basic functions, some derived functions are available for specific calculations:
| Function | Property type | Description | Formula | Required Parameters |
|----------|---------------|-------------|---------|---------------------|
|`avMassVelocity` | bulk | Average velocity weighted by mass | $\frac{\sum_{i \in \text{region}} m_i \cdot v_i}{\sum_{i \in \text{region}} m_i}$ | - |
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### 6.4. Available Fields
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All the pointFields in the simulation database (for in-simulation processing), or the ones stored in the time folders (for post-simulation processing) can be referenced in the operations. In addition to them, some extra fields are available for use in the operations. The following fields are available for use in the operations:
1. Extra fileds to be used in post-processing operations:
| Field | Field Type | Description | Default Value |
|-------|------------|-------------|---------------|
| `position` | `realx3` | Particle positions | - |
| `one` | `real` | Value 1 for each particle | 1 |
| `mass` | `real` | Particle mass | - |
| `density` | `real` | Particle density | - |
| `volume` | `real` | Particle volume | - |
| `diameter` | `real` | Particle diameter | - |
| `I` | `real` | Moment of inertia | - |
2. Common fields which are available in the simulation database/time folders:
| Field | Field Type | Description |
|-------|------------|-------------|
| `velocity` | `realx3` | Particle velocity |
| `rVelocity` | `realx3` | Particle rotational velocity |
| `acceleration` | `realx3` | Particle acceleration |
| `rAcceleration` | `realx3` | Particle rotational acceleration |
| `contactForce` | `realx3` | Particle contact force |
| `contactTorque` | `realx3` | Particle contact torque |
| `id` | `integer` | Particle ID |
| `shapeIndex` | `integer` | Particle shape index |
The above fields may vary from one type of simulation to other. Pleas note that this is only a tentative list.
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### 6.5. Optional Parameters
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| Parameter | Description | Default | Options |
|-----------|-------------|---------|---------|
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| `divideByVolume` | Divide result by region volume | `no` | `yes` or `no` |
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| `threshold` | Exclude regions with fewer particles | 1 | Integer value |
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| `includeMask` | Filter particles based on a field value | `all` | `all` , `lessThan` , `greaterThan` , `between` , `lessThanOrEq` , `greaterThanOrEq` , `betweenEq` |
|`fluctuation2` (in average only)| Calculate fluctuation of field values | `no` | `yes` or `no` |
| `phi` | Field to be used for weighted averaging | `one` | Any valid field name |
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## 7. Examples
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### 7.1. Example 1: Probing Individual Particles
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```cpp
velocityProb
{
processMethod particleProbe;
processRegion centerPoints;
selector id;
field component(position,y);
ids (0 10 100);
timeControl default;
}
```
This example extracts the y-component of the position for particles with IDs 0, 10, and 100.
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### 7.2. Example 2: Processing in a Spherical Region
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```cpp
on_single_sphere
{
processMethod arithmetic;
processRegion sphere;
sphereInfo
{
radius 0.01;
center (-0.08 -0.08 0.015);
}
timeControl default;
operations
(
averageVel
{
function average;
field mag(velocity);
divideByVolume no;
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fluctuation2 yes;
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threshold 3;
includeMask all;
}
par1Fraction
{
function average;
field one;
phi one;
divideByVolume no;
includeMask lessThan;
lessThanInfo
{
field diameter;
value 0.0031;
}
}
numberDensity
{
function sum;
field one;
phi one;
divideByVolume yes;
}
);
}
```
This example defines a sphere region and performs three operations:
1. Calculate the average of velocity magnitude of particles
2. Calculate the fraction of particles with diameter less than 0.0031
3. Calculate the number density by summing and dividing by volume
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### 7.3. Example 3: Processing Along a Line
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In this example, a line region is defined. The `lineInfo` section specifies the start and end points of the line, the number of spheres to create along the line, and the radius of each point. Bulk properties are calculated in each sphere, based on the properties of particles contained in each sphere.
```cpp
along_a_line
{
processMethod arithmetic;
processRegion line;
timeControl simulationTime;
startTime 1.0;
endTime 3.0;
executionInterval 0.1;
lineInfo
{
p1 (0 0 0);
p2 (0 0.15 0.15);
nSpheres 10;
radius 0.01;
}
operations
(
bulkDensity
{
function sum;
field mass;
phi one;
divideByVolume yes;
}
volumeDensity
{
function sum;
field volume;
divideByVolume yes;
}
);
}
```
This example creates 10 spherical regions along a line from (0,0,0) to (0,0.15,0.15) and calculates the bulk density and volume density in each region.
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## 8. Advanced Features
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### 8.1. Special functions applied on fields
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You can access specific components of vector fields (`realx3`) using the `component` function:
```cpp
field component(position,y); // Access the y-component of position
```
Here is a complete list of these special functions:
| Function Name | Valid field Type | Example |
|-----------------|------------|---------|
| `component` | `realx3` | `component(velocity,x)` |
| `abs` | `real` | `abs(s)` |
| `square` | `real` | `square(I)` |
| `cube` | `real` | `cube(diameter)` |
| `squre root` | `real` | `sqrt(mass)` |
| `magnitude` | `realx3` | `mag(contactForce)` |
| `magnitude square` | `realx3` | `magSquare(velocity)` |
| `magnitude cube` | `realx3` | `magCube(velocity)` |
| `magnitude square root` | `realx3` | `magSqrt(acceleration)` |
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### 8.2. Particle Filtering with includeMask
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The `includeMask` parameter allows you to filter particles based on field values:
```cpp
includeMask lessThan;
lessThanInfo
{
field diameter;
value 0.0031;
}
```
Supported masks:
- `all` : Include all particles (default)
- `lessThan` : Include particles where field < value
- `greaterThan` : Include particles where field > value
- `between` : Include particles where value1 < field < value2
- `lessThanOrEq` : Include particles where field ≤ value
- `greaterThanOrEq` : Include particles where field ≥ value
- `betweenEq` : Include particles where value1 ≤ field ≤ value2
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### 8.3. Implementation Notes
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- The postprocessing system can work both during simulation (`runTimeActive yes`) or after simulation completion.
- When using post-simulation mode, you must specify the correct `shapeType` to properly initialize the shape objects.
- Results are written to output files in the case directory with timestamps.
- The `threshold` parameter helps eliminate statistical noise in regions with few particles.
- Setting `divideByVolume` to `yes` normalizes results by the volume of the region, useful for calculating densities.
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## 9. Mathematical Formulations
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For weighted `bulk` properties calculation, we have these two general formulations:
- For weighted averaging:
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$$ \text{average} = \frac{\sum_j w_j \cdot \phi_j \cdot \text{field}_j}{\sum_i w_i \cdot \phi_i} $$
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- For weighted summing:
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$$ \text{sum} = \sum_j w_j \cdot \phi_j \cdot \text{field}_j $$
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If `divideByVolume` is set to `yes` , the result is divided by the volume of the region:
$$ \text{volumetric result} = \frac{\text{result}}{V_{\text{region}}} $$
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## 10. A complete dictioanry file (postprocessDataDict)
```C++
/* -------------------------------*- C++ -*--------------------------------- *\
| phasicFlow File |
| copyright: www.cemf.ir |
\* ------------------------------------------------------------------------- */
objectName postprocessDataDict;
objectType dictionary;;
fileFormat ASCII;
/*---------------------------------------------------------------------------*/
// Yes: postprocessing is active during the simulation
// No: postprocessing is not active during the simulation
// and it can be done after simulation
runTimeActive yes;
// shapeType: defines the type of the shape that is used in the simulation
// (for example: sphere, grain, etc).
// shapeType is only used when postprocessing is done after simulation
// to initialize the shape object for post processing operatoins
shapeType sphere;
// default time control to be used in the postprocessing components
defaultTimeControl
{
timeControl timeStep; // timeStep, simulationTime are the options here
startTime 0;
endTime 1000;
executionInterval 150;
}
// list of postprocessing components
components
(
// probing particles for their state variables, like velocity, position, etc
velocityProb
{
processMethod particleProbe;
processRegion centerPoints;
selector id;
field component(position,y);
ids (0 10 100);
timeControl default; // other options are settings, timeStep, simulationTime
// settings: uses parameters from settingsDict file
// timeStep: uses the time step of the simulation controlling the execution of postprocessing
// simulationTime: uses the simulation time of the simulation controlling the execution of postprocessing
// default: uses the default time control (defined in defaultTimeControl).
// default behavior: if you do not specify it, parameters in defaultTimeControl is used.
}
on_single_sphere
{
// method of performing the sum (arithmetic, uniformDistribution, GaussianDistribution)
processMethod arithmetic;
// Postprocessing is done on particles whose centers are inside this spehre
processRegion sphere;
sphereInfo
{
radius 0.01; // radius of sphere
center (-0.08 -0.08 0.015); // center of sphere
}
timeControl default;
/// all the postprocess operations to be done on sphere region
operations
(
// computes the arithmetic mean of particle velocity
averageVel
{
function average;
field velocity;
fluctuation2 yes;
divideByVolume no; // default is no
threshold 3; // default is 1
includeMask all; // default is all
}
// - function: average, sum, and other derived ones from sum and average
// - field: names of the fields in the simulation. Some special fields
// are: mass, density, volume, position, one, I.
// - divideByVolume: whether the result is divided by the volume of the region
// - threshold: exclude regions that contains particles less than threshold
// - includeMask: all, lessThan, greaterThan, between, lessThanOrEq, greaterThanEq, betweenEq
// computes the fraction of par1 in the region
par1Fraction
{
function average;
field one; // default
phi one; // default
divideByVolume no;
includeMask lessThan;
// diameter of par1 is 0.003, so these settings
// will select only particles of type par1
lessThanInfo
{
field diameter;
value 0.0031;
}
}
numberDensity
{
function sum;
field one;
phi one;
divideByVolume yes;
}
);
}
along_a_line
{
processMethod arithmetic;
processRegion line;
// the time interval for executing the post-processing
// other options: timeStep, default, and settings
timeControl simulationTime;
startTime 1.0;
endTime 3.0;
executionInterval 0.1;
// 10 spheres with radius 0.01 along the straight line defined by p1 and p2
lineInfo
{
p1 (0 0 0);
p2 (0 0.15 0.15);
nSpheres 10;
radius 0.01;
}
operations
(
// computes the arithmetic mean of particle velocity
numberDensity
{
function sum;
field one;
divideByVolume yes; //default is no
}
volumeDensity
{
function sum;
field volume; //
divideByVolume yes; //default is no
}
);
}
);
```