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|`low_Mach`| Integer | Low Mach number correction for HLLC Riemann solver: [0] None; [1] Pressure (Chen et al. 2022); [2] Velocity (Thornber et al. 2008) |
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|`avg_state`| Integer | Averaged state evaluation method: [1] Roe average*; [2] Arithmetic mean |
@@ -476,7 +482,14 @@ It is recommended to set `weno_eps` to $10^{-6}$ for WENO-JS, and to $10^{-40}$
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-`mp_weno` activates monotonicity preservation in the WENO reconstruction (MPWENO) such that the values of reconstructed variables do not reside outside the range spanned by WENO stencil ([Balsara and Shu, 2000](references.md); [Suresh and Huynh, 1997](references.md)).
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-`riemann_solver` specifies the choice of the Riemann solver that is used in simulation by an integer from 1 through 3.
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-`muscl_order` specifies the order of the MUSCL scheme that is used for spatial reconstruction of variables by an integer of 1, or 2, that corresponds to the 1st, and 2nd order respectively. When using `muscl_order = 2`, `muscl_lim` must be defined.
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-`muscl_lim` specifies the slope limiter that is used in 2nd order MUSCL Reconstruction by an integer from 1 through 5.
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`muscl_lim = 1`, `2`, `3`, `4`, and `5` correspond to minmod, monotonized central, Van Albada, Van Leer, and SUPERBEE, respectively.
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-`int_comp` activates interface compression using THINC used in MUSCL Reconstruction, with control parameters (`ic_eps`, and `ic_beta`).
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-`riemann_solver` specifies the choice of the Riemann solver that is used in simulation by an integer from 1 through 4.
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`riemann_solver = 1`, `2`, and `3` correspond to HLL, HLLC, and Exact Riemann solver, respectively ([Toro, 2013](references.md)).
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`riemann_solver = 4` is only for MHD simulations. It resolves 5 of the full seven-wave structure of the MHD equations ([Miyoshi and Kusano, 2005](references.md)).
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@@ -576,6 +589,7 @@ To restart the simulation from $k$-th time step, see [Restarting Cases](running.
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|`omega_wrt(i)`| Logical | Add the $i$-direction vorticity to the database |
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|`schlieren_wrt`| Logical | Add the numerical schlieren to the database|
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|`qm_wrt`| Logical | Add the Q-criterion to the database|
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|`liutex_wrt`| Logical | Add the Liutex to the database|
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|`tau_wrt`| Logical | Add the elastic stress components to the database|
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|`fd_order`| Integer | Order of finite differences for computing the vorticity and the numerical Schlieren function [1,2,4]|
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|`schlieren_alpha(i)`| Real | Intensity of the numerical Schlieren computed via `alpha(i)`|
@@ -615,7 +629,7 @@ If `file_per_process` is true, then pre_process, simulation, and post_process mu
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-`output_partial_domain` activates the output of part of the domain specified by `[x,y,z]_output%beg` and `[x,y,z]_output%end`.
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This is useful for large domains where only a portion of the domain is of interest.
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It is not supported when `precision = 1` and `format = 1`.
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It also cannot be enabled with `flux_wrt`, `heat_ratio_wrt`, `pres_inf_wrt`, `c_wrt`, `omega_wrt`, `ib`, `schlieren_wrt`, or `qm_wrt`.
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It also cannot be enabled with `flux_wrt`, `heat_ratio_wrt`, `pres_inf_wrt`, `c_wrt`, `omega_wrt`, `ib`, `schlieren_wrt`, `qm_wrt`, or 'liutex_wrt'.
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