KHRT Droplet Breakup Model Reference
The KHRT Breakup model combines two submodels, one based on Kelvin-Helmholtz (KH) theory and one based on Rayleigh-Taylor (RT) theory.
Both breakup submodels consider the growth of instabilities on a droplet and provide expressions for their wavelength and frequency. Kelvin-Helmholtz instabilities are due to the slip velocity of the droplet, which eventually shears small child droplets off the parent [688], corresponding to the stripping regime. Rayleigh-Taylor instabilities are due to the acceleration of the droplet and tend to shatter the droplet completely [683], corresponding to the catastrophic regime. The KH and RT submodels compete: instabilities due to both can grow simultaneously; if they grow for long enough, breakup occurs due to the RT instabilities. Otherwise KH breakup occurs.
Theory | See KHRT Breakup Model. | ||
Provided By | |||
Example Node Path | |||
Requires |
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Properties | Key properties are: Child Parcels. See KHRT Breakup Properties. | ||
Activates | Materials | See KHRT Breakup Material Properties. | |
Field Functions | Droplet Dynamic Viscosity, Droplet Surface Tension, Droplet Weber Number. See KHRT Breakup Field Functions. |
KHRT Breakup Properties
- Child Parcels
- Number of child parcels to create during a breakup event.
- Normal Velocity Coefficient
- Normal velocity coefficient for child parcels, in Eqn. (3101)
- B0
- KH length coefficient, Eqn. (3099)
- B1
- KH time coefficient, Eqn. (3098)
- C3
- RT length coefficient, Eqn. (3104)
- Ctau
- RT time coefficient, Eqn. (3103)
- Maximum fractional shed mass
- Maximum fraction of the parcel mass that is shed before the child parcels are created.
KHRT Breakup Material Properties
- Dynamic Viscosity
- The dynamic viscosity of the droplet.
- Surface Tension
- The droplet surface tension .
KHRT Breakup Field Functions
- Droplet Dynamic Viscosity
- The dynamic viscosity of the droplet .
- Droplet Surface Tension
- The surface tension of the droplet .
- Droplet Weber Number
- The droplet Weber number in Eqn. (3093).