In a nutshell, the equation integrated governs a set of scalars, , , as
with parameter vectors , , and . This is the same as in DiffEq/Beta.h. Here is an isotropic vector-valued Wiener process with independent increments. The invariant distribution is the joint beta distribution. This system of SDEs consists of N independent equations. For more on the beta SDE, see https://doi.org/10.1080/14685248.2010.510843.
In addition to integrating the above SDE, there are two additional functions of are computed as
These equations compute the instantaneous mixture density, , and instantaneous specific volume, , for equation in the system. These quantities are used in binary mixing of variable-density turbulence between two fluids with constant densities, and . The additional parameters, and are user input parameters and kept constant during integration. Since we compute the above variables, and , and call them mixture density and specific volume, respectively, , governed by the beta SDE is a mass fraction, hence the name mass-fraction beta.
All of this is unpublished, but will be linked in here once published.
Search for symbols, directories, files, pages or modules. You can omit any
prefix from the symbol or file path; adding a : or /
suffix lists all members of given symbol or directory. Navigate through the
list using ↓ and
Enter to go.