S-Gamma Models Reference
The S-Gamma model is a phase model for particle size distribution.
The S-Gamma model (see Lo and Rao [505], and Lo and Zhang [507]) is based on predicting the transport of the moments of the particle size distribution:
- Zeroth moment: the particle number density, .
- Second moment: related to the interfacial area density.
- Third moment: related to the dispersed phase volume fraction.
One transport equation is solved for each moment. As the third moment is based on the dispersed phase volume fraction, it can be derived from the volume fraction equation that is solved by the Segregated EMP Flow solver. You can choose whether to solve for just the second moment, or for the zeroth and second moments, by selecting the required option in the properties of the S-Gamma model. Extensions to the S-Gamma model can be supplied using the source terms for the zeroth and second moments.
Two S-Gamma implementations are provided:
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Discrete Quadrature S-Gamma
This model evaluates the integrals associated with breakup, coalescence and bubble entrainments using an adaptive discrete quadrature method.
If the One-Equation option is selected, the integrals are evaluated using a one-point integration at . If the Two-Equation option is selected, the integration points are distributed log-normally with the appropriate , and .
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Pre-Integrated S-Gamma
This model evaluates the integrals using an analytical method.
If you wish to include the effects of breakup and coalescence on the predicted size distribution, you can select the S-Gamma Breakup and S-Gamma Coalescence models in a multiphase interaction that includes the dispersed phase.
When simulating multiple flow regime flows, if you wish to model the size of newly created bubbles/droplets, you can select the S-Gamma Entrainment model.
Breakup/coalescence or entrainment interaction models for multiple flow regimes are only available with the Discrete Quadrature S-Gamma implementation in a multiphase interaction.
Model Names | Discrete Quadrature S-Gamma | ||
Pre-Integrated S-Gamma | |||
Theory | See S-Gamma Model for Particle Size Distribution. | ||
Provided By |
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Example Node Path | |||
Requires |
Create two phases. This model is used only in the dispersed phase. Phase model selection (deactivate the Auto-select recommended models checkbox):
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Properties | Key properties are: We Crit and Number of S-Gamma Equations. | ||
Activates | Physics Models |
S-Gamma Breakup and S-Gamma Coalescence are activated as optional models in a Continuous-Dispersed phase interaction when the dispersed phase has the S-Gamma model activated, or in a Multiple Flow Regime phase interaction when one of the phases has the S-Gamma model activated. The S-Gamma Entrainment is activated as an optional model in a Multiple Flow Regime phase interaction when one of the phases has the S-Gamma model activated See Discrete Quadrature S-Gamma Phase Interaction Model Reference and Pre-Integrated S-Gamma Phase Interaction Model Reference. |
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Model Controls (child nodes) |
S-Gamma Turbulent Prandtl Number See Model Controls. |
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Initial Conditions |
Size Distribution Specification
See Initial Conditions. |
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Boundary Inputs |
Size Distribution Specification
See Boundary Settings. |
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Region Inputs |
S-Gamma Source Option
See Region Settings. |
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Solvers | S-Gamma | ||
Field Functions | See S-Gamma Model Field Functions. |
S-Gamma Model Properties
- Minimum Diameter
- Sets the minimum allowed Sauter mean diameter.
- Maximum Diameter
- Sets the maximum allowed Sauter mean diameter.
- Number of S-Gamma Equations
- Selects the number of extra
equations to solve in addition to the volume fraction.
- One
Equation
Solves for the transport of interfacial area density (the second moment, in Eqn. (2185)).
- Two
Equation
Solves for both the transport of particle number density and the interfacial area density (zeroth and second moments, in Eqn. (2180) and in Eqn. (2185)).
Note When the Fluid Film Wave Stripping or Edge Stripping model is activated, only the Two Equation option is available. - One
Equation
- Convection
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Specifies the order of approximation of the convection term used in the S-Gamma transport equations. See Eqn. (2190) and Eqn. (2194).
- 1st-order
Selects the first-order convection scheme.
- 2nd-order
Selects the second-order convection scheme.
- 1st-order
- Number of Quadrature Points
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Quadrature points are the sample values on the curve on which the numerical integration is performed. A larger number of points can produce more accurate results, but requires more calculations and so takes longer to perform.
You can specify any number of points. However, the default value of 5 is suitable for most purposes.
- Secondary Gradients
- Neglect or include the boundary secondary gradients for
diffusion and/or the interior secondary gradients at mesh faces.
- On: Include both secondary gradients.
- Off: Exclude both secondary gradients.
- Interior Only: Include the interior secondary gradients only.
- Boundaries Only: Include the boundary secondary gradients only.
Model Controls
The following child node is available for Pre-Integrated S-Gamma and Discrete Quadrature S-Gamma models with turbulent viscous regimes only.
- S-Gamma Turbulent Prandtl Number
- Sets the ratio of kinematic turbulent viscosity and coefficient of turbulent diffusion of the S-Gamma moments. This value is in Eqn. (2189).
Initial Conditions
- Size Distribution Specification
- Sets the initial particle size distribution in the dispersed phase and controls whether to include particle size variance in the calculations.
Boundary Settings
- Inlets and Pressure Boundaries
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- Size Distribution Specification
- Sets the initial particle size distribution in the dispersed phase and controls whether to include particle size variance in the calculations.
Region Settings
Applies to the dispersed phase in a fluid region.
- S-Gamma Source Option
- Provides access to the and source terms.
S-Gamma Solver Properties
The S-Gamma solver controls the solution update for the S-Gamma model.
You are advised to use the same relaxation factor settings for this solver and the Volume Fraction solver.
The properties in the Expert category are for a temporary debug situation, at the expense of simulation accuracy and higher memory usage. Do not change these properties unless you are thoroughly familiar with the Simcenter STAR-CCM+ discretization techniques.
- Implicit Under-Relaxation Factor
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Improves stability and convergence of the linear system by using the relaxation factor to increase diagonal dominance of the matrix.
The default value is 0.5.
- Explicit Under-Relaxation Factor
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Specifies the multiplier that is applied to the provisional increment of the solution. Sharing the relaxation between implicit and explicit factors can be used to improve performance.
The default value is 1.0.
- Overall Relaxation Factor
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The product of the two under-relaxation factors (that is, Implicit Under-Relaxation Factor times Explicit Under-Relaxation Factor). This (read-only) value is a guide to the combined effect of the relaxation.
- Interaction Source Storage Retained
- When activated, interaction source storage is retained at the end of the iteration. The breakup and coalescence source terms are made available as field functions.
To understand how breakup and coalescence are working in a particular application, you can examine their contributions to the and transport equations (Eqn. (2185) and Eqn. (2194) respectively).
- Reconstruction Frozen
- When On, Simcenter STAR-CCM+ does not update reconstruction gradients with each iteration, but rather uses gradients from the last iteration in which they were updated. Activate Temporary Storage Retained in conjunction with this property. This property is Off by default.
- Reconstruction Zeroed
- When On, the solver sets reconstruction gradients to zero at the next iteration. This action means that face values used for upwinding (Eqn. (905)) and for computing cell gradients (Eqn. (917) and Eqn. (918)) become first-order estimates. This property is Off by default. If you turn this property Off after having it On, the solver recomputes the gradients on the next iteration.
- Solver Frozen
- When On, the solver does not update any quantity during an iteration. It is Off by default. This is a debugging option that can result in non-recoverable errors and wrong solutions due to missing storage. See Finite Volume Solvers Reference for details.
- Temporary Storage Retained
- When On, Simcenter STAR-CCM+ retains additional field data that the solver generates during an iteration. The particular data retained depends on the solver, and becomes available as field functions during subsequent iterations. Off by default.
S-Gamma Model Field Functions
The following field functions are made available to the simulation when the S-Gamma model is used.
- ParticleSizeVariance of [phase]
- in Eqn. (2182).
- SauterMeanDiameter of [phase]
- in Eqn. (2181), Eqn. (2182), and Eqn. (2183).
- SecondSizeDistributionMoment of [phase]
- in Eqn. (2179), Eqn. (2183), and Eqn. (2194).
- ThreeZeroDiameter of [phase]
- in Eqn. (2181), Eqn. (2182), and Eqn. (2183).
- ZerothSizeDistributionMoment of [phase]
- in Eqn. (2172), Eqn. (2171), Eqn. (2183), and Eqn. (2185).