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|`alt_soundspeed` * | Logical | Alternate sound speed and $K \nabla \cdot u$ for 5-equation model |
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|`adv_alphan`| Logical | Equations for all $N$ volume fractions (instead of $N-1$) |
@@ -323,6 +325,7 @@ Details of implementation of viscosity in MFC can be found in [Coralic (2015)](r
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-\* Options that work only with `model_eqns` $=2$.
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- † Options that work only with `cyl_coord` $=$ `False`.
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- ‡ Options that work only with `bc_[x,y,z]%[beg,end] = -15` and/or `bc_[x,y,z]%[beg,end] = -16`
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The table lists simulation algorithm parameters.
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The parameters are used to specify options in algorithms that are used to integrate the governing equations of the multi-component flow based on the initial condition.
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-`bc_[x,y,z]%[beg,end]` specifies the boundary conditions at the beginning and the end of domain boundaries in each coordinate direction by a negative integer from -1 through -12.
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See table [Boundary Conditions](#boundary-conditions) for details.
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-`bc_[x,y,z]\%vb[1,2,3]` specifies the velocity in the (x,1), (y,2), (z,3) direction applied to `bc_[x,y,z]%beg` when using `bc_[x,y,z]%beg = -16`.
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Tangential velocities require viscosity, `weno_avg = T`, and `bc_[x,y,z]%beg = -16` to work properly. Normal velocities require `bc_[x,y,z]\%end = -15` or `\bc_[x,y,z]\%end = -16` to work properly.
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-`bc_[x,y,z]\%ve[1,2,3]` specifies the velocity in the (x,1), (y,2), (z,3) direction applied to `bc_[x,y,z]%beg` when using `bc_[x,y,z]%end = -16`.
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Tangential velocities require viscosity, `weno_avg = T`, and `bc_[x,y,z]\%end = 16` to work properly. Normal velocities require `bc_[x,y,z]\%end = -15` or `\bc_[x,y,z]\%end = -16` to work properly.
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-`model_eqns` specifies the choice of the multi-component model that is used to formulate the dynamics of the flow using integers from 1 through 3.
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`model_eqns` $=$ 1, 2, and 3 correspond to $\Gamma$-$\Pi_\infty$ model ([Johnsen, 2008](references.md#Johnsen08)), 5-equation model ([Allaire et al., 2002](references.md#Allaire02)), and 6-equation model ([Saurel et al., 2009](references.md#Saurel09)), respectively.
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The difference of the two models is assessed by ([Schmidmayer et al., 2019](references.md#Schmidmayer19)).
Reference: Bezgin, D. A., & Buhendwa A. B., & Adams N. A. (2022). JAX-FLUIDS: A fully-differentiable high-order computational fluid dynamics solver for compressible two-phase flows. arXiv:2203.13760
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Reference: Ghia, U., & Ghia, K. N., & Shin, C. T. (1982). High-re solutions for incompressible flow
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using the Navier-Stokes equations and a multigrid method. Journal of Computational Physics, 48, 387-411
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