Additional right-hand side source terms for velocity components equation (Navier-Stokes)
Local variables and initialization
double cs_real_t
Floating-point value.
Definition cs_defs.h:302
int cs_lnum_t
local mesh entity id
Definition cs_defs.h:298
cs_field_t * cs_field_by_id(int id)
Return a pointer to a field based on its id.
Definition cs_field.c:2307
@ rho
Definition cs_field_pointer.h:103
#define CS_F_(e)
Macro used to return a field pointer by its enumerated value.
Definition cs_field_pointer.h:51
cs_mesh_quantities_t * cs_glob_mesh_quantities
Field descriptor.
Definition cs_field.h:124
cs_real_t * cell_vol
Definition cs_mesh_quantities.h:93
cs_lnum_t n_cells
Definition cs_mesh.h:73
Example
Example of arbitrary source term for component
:
appearing in the equation under the form:

In the following example:
with:
CKP = 1.0 (in
) (return term on velocity)
MMT = 100.0 (in
) (momentum production by volume and time unit)
which yields:
st_imp[i][0][0] = volume[i] * A = - volume[i]*(rho*CKP)
st_exp[i][0] = volume[i] * B = volume[i]*(XMMT)
Body
_st_imp[i][0][0] = - cell_f_vol[i] * cpro_rom[i] * ckp;
_st_exp[i][0] = cell_f_vol[i] * cpro_rom[i] * xmmt;
}
}
cs_real_t cs_real_3_t[3]
vector of 3 floating-point values
Definition cs_defs.h:315
cs_real_t cs_real_33_t[3][3]
3x3 matrix of floating-point values
Definition cs_defs.h:321
@ vel
Definition cs_field_pointer.h:68
Example of a boussinesq momentum source term
Example to add Boussinesq source to the z component of
:
Body
_st_exp[c_id] = cell_f_vol[c_id] * rh0 * beta * (cvar_temperature[i]-t0);
}
}
@ t
Definition cs_field_pointer.h:98
const cs_fluid_properties_t * cs_glob_fluid_properties
Definition cs_physical_constants.c:346
double ro0
Definition cs_physical_constants.h:72
double t0
Definition cs_physical_constants.h:78