# controls_dev

Warning

CONTAINS OPTIONS THAT HAVE NOT YET BEEN THE GIVEN A GREEN LIGHT FOR GENERAL USE. IN PARTICULAR, THESE ARE NOT YET FOR USE IN RESEARCH TO BE PUBLISHED.

## TDC options

```
compare_TDC_to_MLT = .false.
```

## RSP2 parameters

RSP2 time weighting is determined by the velocity_time_centering controls.

for Pt and Lt in turbulent energy equation

for P and grav in momentum equation

for P and L in energy equation

for area when multiplied by P

RSP2_Lsurf_factor: Lsurf = RSP2_Lsurf_factor*area(1)*clight*crad*T(1)**4 RSP2_use_Stellingwerf_Lr as in RSP

```
RSP2_alfad = 1.0d0
RSP2_alfap = 0.0d0
RSP2_alfat = 0.0d0
RSP2_alfam = 0.25d0
RSP2_alfar = 0.0d0
RSP2_min_Lt_div_L_for_overshooting_mixing_type = 1d-4
RSP2_min_Lc_div_L_for_convective_mixing_type = 1d-4
RSP2_Lsurf_factor = 0.5d0
RSP2_report_adjust_w = .false.
RSP2_use_L_eqn_at_surface = .true.
RSP2_assume_HSE = .true.
RSP2_use_RSP_eqn_for_Y_face = .true.
RSP2_use_mass_interp_face_values = .false.
RSP2_use_Stellingwerf_Lr = .true.
RSP2_num_outermost_cells_forced_nonturbulent = 0
RSP2_num_innermost_cells_forced_nonturbulent = 0
RSP2_w_fix_if_neg = 5d-5
RSP2_w_min_for_damping = 1d2
RSP2_source_seed = 0d0
RSP2_remesh_when_load = .true.
RSP2_nz = 150
RSP2_nz_outer = 40
RSP2_T_anchor = 11d3
RSP2_dq_1_factor = 2d0
RSP2_nz_div_IBOTOM = 30d0
```

period controls

```
RSP2_target_steps_per_cycle = 600
RSP2_min_max_R_for_periods = -1
```

when to stop

```
RSP2_max_num_periods = -1
RSP2_GREKM_avg_abs_frac_new = 0.1d0
RSP2_GREKM_avg_abs_limit = -1
```

output data for work integrals during a particular period

```
RSP2_work_period = -1
RSP2_work_filename = 'work.data'
```

output data for 3d map. format same as for gnuplot pm3d

```
RSP2_write_map = .false.
RSP2_map_columns_filename = 'map_columns.list'
```

items listed in your map columns must also appear in your profile columns

```
RSP2_map_filename = 'map.data'
RSP2_map_first_period = -1
RSP2_map_last_period = -1
RSP2_map_zone_interval = 2
RSP2_map_history_filename = 'map_history.data'
```

### mass corrections

## use_mass_corrections

Gravitational vs baryonic mass corrections.

The Lagrangian coordinate (\(m\)) in MESA is the baryonic mass and the density (\(\rho\)) is the baryonic mass density.

If false, then no distinction between gravitational and baryonic mass. If true, then the gravitational mass is calculated using mass corrections and the momentum equation, total energy equation, and Brunt are modified.

The variable `mass_correction`

is the quantity you multiply
the baryonic mass density by to get the gravitational mass
density:

(mass density) = (baryon density) * amu * mass_correction

Given the mass fractions in a cell, the value of
mass_correction is provided by the `chem`

module.

MESA holds m_grav fixed during the newton iterations. This results in an energy conservation error, because the specific potential energy changes when m_grav is updated afterwards. A message showing the relative energy error incurred due to this assumption will be printed to the terminal.

Not compatible with RSP.

```
use_mass_corrections = .false.
```

## phase_separation_no_diffusion

if true and element diffusion is on, prevent element diffusion from occurring in the layers where phase separation mixing is present (experimental)

```
phase_separation_no_diffusion = .false.
```

### split burn

## op_split_burn_min_T_for_variable_T_solver

use variable T, constant density solver for op_split_burn in cells with T >= this limit at start of step. only adopted in cells with T >= op_split_burn_min_T at start of step.

```
op_split_burn_min_T_for_variable_T_solver = 1d99
```