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| class | collisionPhaseTransfer |
| | Model to represent the absorption of droplets or bubbles into a corresponding Eulerian phase as a result of collisions with that phase (and potentially other non-carrier Eulerian phases). This can be used to represent (e.g.) a spray of droplets hitting and being absorbed by a VoF interface. The collision probability is calculated as proportional to the Eulerian phase's surface area per unit volume and the distance travelled by the particle. More...
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| class | constantCoefficientVirtualMass |
| | Constant-coefficient virtual mass model. More...
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| class | constantFluxCarrierTransfer |
| | Model to represent mass transfer into the carrier phase with a constant surface volume or mass flux. This model provides a crude approximation of phase change which neglects any thermal effects. It can be used by clouds and in solvers that do not feature any thermodynamic modelling. More...
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| class | diskInjection |
| | Disk injection model. This injects particles continuously over a disk with a given number rate. The disk is characterised by a centre, and axis and an inner and an outer diameter. The centre and axis and number rate are all Function1-s and can vary with time. More...
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| class | drag |
| | Base class for Lagrangian drag models. More...
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| class | GidaspowErgunWenYuDrag |
| | Drag model of Gidaspow which switches between the drag models of Ergun and Wen and Yu at different particulate volume dractions. More...
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| class | gravity |
| | Gravity force model. More...
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| class | heatTransfer |
| | Base class for Lagrangian heat transfer models. More...
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| class | manualInjection |
| | Manual injection model. This injects particles instantaneously at a list of positions specified in a separate file. More...
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| class | patchInjection |
| | Patch injection model. This injects particles continuously at a patch with a given number rate. The number rate is a Function1 and can vary with time. More...
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| class | pointInjection |
| | Point injection model. This injects particles continuously at a point with a given number rate. The point and the number rate are both Function1-s and can both vary with time. More...
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| class | pressureGradientForce |
| | Pressure gradient force model. More...
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| class | pressureWork |
| | Model for pressure work. Subtracts the pressure-volume work associated with particle expansion from the particle energy, and adds it to the carrier energy. This model is needed to make (e.g.,) bubbles reduce in temperature as they expand. More...
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| class | RanzMarshallHeatTransfer |
| | Heat transfer model of Ranz and Marshall for spherical particles in a turbulent carrier flow. More...
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| class | SaffmanMeiLift |
| | Lift model of Saffman (1965) as extended by Mei (1992). Applicable to spherical particles. More...
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| class | SchillerNaumannDrag |
| | Drag model of Schiller and Naumann for spherical particles in a turbulent carrier flow. More...
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| class | turbulentDispersion |
| | Model for turbulent dispersion. This model creates a random turbulent velocity fluctuation based on the carrier's turbulent properties. It then uses the drag model to construct a corresponding force which it applies for a duration equal to the carrier's turbulent time scale. More...
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| class | volumeInjection |
| | Volume injection model. This injects particles instantaneously within the volume of a set of cells. Particles are positioned randomly. More...
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| class | accumulationScheme |
| | Basic cell Lagrangian accumulation scheme. More...
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| class | ddtScheme |
| | Abstract base class for Lagrangian ddt schemes. More...
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| class | SpScheme |
| | Abstract base class for Lagrangian Sp schemes. More...
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