Reitz-Diwakar Droplet Breakup Model Reference
The Reitz-Diwakar Breakup model is based on observed length- and time-scales of droplet breakup.
The Reitz-Diwakar breakup model, [689] and [690], assumes that breakup occurs in one of two possible modes:
- Bag breakup, in which the non-uniform pressure field around the droplet causes it to expand in the low-pressure wake region and eventually disintegrate when surface tension forces are overcome.
- Stripping breakup, in which liquid is sheared or stripped from the droplet surface.
The model calculates local disturbances on a cylindrical free surface and traces the growth rate of the most unstable mode. It does not generate child parcels, hence it is computationally efficient to run. It can be used to estimate the importance of breakup before turning to a more complex model, or to provide support to conclusions obtained from such a model.
Theory | See Reitz-Diwakar Breakup Model. | ||
Provided By | |||
Example Node Path | |||
Requires |
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Properties | Key properties are: WeCrit. See Reitz-Diwaker Breakup Properties. | ||
Activates | Materials | See Reitz-Diwaker Breakup Material Properties. | |
Field Functions | Droplet Surface Tension, Droplet Weber Number. See Reitz-Diwaker Breakup Field Functions. |
Reitz-Diwaker Breakup Properties
- WeCrit
- Minimum Weber number for breakup, see Eqn. (3106).
- Cb2
- Bag breakup time-scale coefficient, see Eqn. (3109).
- Cs1
- Coefficient prescribing the onset of stripping breakup, see Eqn. (3108).
- Cs2
- Stripping breakup time-scale coefficient, see Eqn. (3109).
Reitz-Diwaker Breakup Material Properties
- Surface Tension
- The droplet surface tension .
Reitz-Diwaker Breakup Field Functions
- Droplet Surface Tension
- The surface tension of the droplet .
- Droplet Weber Number
- The droplet Weber number in Eqn. (3093).