Simulate with complex geometries and complex physics
LIQUID
indices for the implicit (incompressible/weakly compressible) solver
The indices here might be also used for other solvers.
| List of members: | |
|---|---|
| %ind_ahc_lh% | latent heat contribution in the apparent heat capacity method |
| %ind_ahc_u% | specific internal energy (in J/kg) |
| %ind_alpha% | |
| %ind_betaDarcy% | porous material coupling parameter, unit: 1/s |
| %ind_BNDpnt_of_pnt_nearBND% | index of closest boundary point for all points which are close to boundary |
| %ind_c% | correction pressure due to projecting the velocity field onto correct div(v) values [Pa] |
| %ind_cD% | |
| %ind_CV% | specific heat capacity (at constant volume), unit: J/(kg*K) |
| %ind_CV_LatentHeat% | |
| %ind_d30% | |
| %ind_DarcyVersion% | How to compute the source terms of the Darcy contributions in the pressure equations |
| %ind_DiagPcorr% | compressibility of the fluid |
| %ind_diss% | energy dissipation due to viscous work [W/kg] |
| %ind_div% | measured, instantaneous divergence of velocity |
| %ind_div_bar% | compression rate due to given temperature or hydrostatic pressure or density time change rate |
| %ind_div_bar_0% | compression rate at the previous time step |
| %ind_div_bar_c% | PURE POSTPROCESSING: the (divergence of velocity)^bar at the point in the numerical scheme where the correction pressure is computed |
| %ind_div_bar_pDyn% | PURE POSTPROCESSING: the (divergence of velocity)^bar at the point in the numerical scheme where the correction pressure is computed |
| %ind_div_tild% | divergence of preliminary velocity |
| %ind_divS(1)% | divergence of solid stress tensor, x-component [Pa/m] |
| %ind_divS(2)% | divergence of solid stress tensor, y-component [Pa/m] |
| %ind_divS(3)% | divergence of solid stress tensor, z-component [Pa/m] |
| %ind_divSe(1)% | divergence of elastic solid stress tensor, x-component [Pa/m] |
| %ind_divSe(2)% | divergence of elastic solid stress tensor, y-component [Pa/m] |
| %ind_divSe(3)% | divergence of elastic solid stress tensor, z-component [Pa/m] |
| %ind_divV_sw% | |
| %ind_divV_transport% | divergence of the transport velocity, internally used for EULER applications |
| %ind_dt_store% | variable for storing the intermediate time step size in case of subcyclings in Eulerian framework |
| %ind_dt_virt% | value of the current local virtual time step size [s] |
| %ind_dtbp% | distance to closest boundary point |
| %ind_eps% | k-epsilon model: turbulent dissipation [m^2/s^3] |
| %ind_eps_dot% | Equivalent tensile/von-Mises (viscous) stress [Pa] |
| %ind_eps_plastic% | plastic deformation, accumulated over time |
| %ind_eps_plastic_dot% | current time change rate of the plastic deformation [1/s] |
| %ind_eps_plastic_dot_dot% | |
| %ind_eps_plastic_v% | volumetric part of the plastic strains (experimental) |
| %ind_ETA% | viscosity, unit: Pa*s |
| %ind_ETA_eff% | effective dynamic viscosity (sum of laminar and turbulent viscosities), unit: Pa*s |
| %ind_ETA_sm% | total viscosity, consisting of physical, turbulent, and additional numerical viscosities; unit: Pa*s |
| %ind_g(1)% | |
| %ind_g(2)% | |
| %ind_g(3)% | |
| %ind_hwf_3d% | |
| %ind_k% | k-epsilon model: turbulent kinetic energy [m^2/s^2] |
| %ind_KEPS_C1% | k-epsilon turbulence model: value of C1 for epsilon computation |
| %ind_KEPS_C2% | k-epsilon turbulence model: value of C2 for epsilon computation |
| %ind_KEPS_cMue% | k-epsilon turbulence model: value of c_{mue} for viscosity computation |
| %ind_KEPS_G% | k-epsilon turbulence model: production term G |
| %ind_LAM% | heat conductivity, unit: W/(m*K) |
| %ind_lap_vn% | |
| %ind_LatentHeat% | |
| %ind_logVi_ist(1)% | time-integrated local defect volume |
| %ind_logVi_ist(2)% | time-integrated relative local defect volume |
| %ind_logVi_soll% | time-integrated relative required volume |
| %ind_MomSrc(1)% | |
| %ind_MomSrc(2)% | |
| %ind_MomSrc(3)% | |
| %ind_MUE% | shear modulus, unit: N/m^2 |
| %ind_MUE_mean% | average shear modulus, computed in case of using Johnson-Cook or yield stress formulations |
| %ind_MUE_relax% | the elastic shear modulus used for relaxation of the material (decreasing norm of stress tensor) |
| %ind_MUE_sm% | shear modulus, after numerical smoothing, unit: N/m^2 |
| %ind_NUE_turb% | turbulent kinematic viscosity, unit m^2/s |
| %ind_p% | hydrostatic pressure |
| %ind_p_0% | hydrostatic pressure at previous time step |
| %ind_p_consolidation% | consolidation pressure in the Camclay model (experimental) |
| %ind_p_corr% | This index is deprecated. Please use ind_p_dyn for the same functionality. |
| %ind_p_corr_0% | This index is deprecated. Please use ind_p_dyn_0 for the same functionality |
| %ind_p_dyn% | dynamic pressure |
| %ind_p_dyn_0% | dynamic pressure at previous time step |
| %ind_pDivV% | prospective new dynamic bubble pressure dereived from implicit algorithms |
| %ind_penalty% | |
| %ind_PenV% | |
| %ind_PHI% | |
| %ind_pnt_nearBND% | mark MESHFREE points near boundary |
| %ind_PSI% | |
| %ind_r% | density, unit: kg/m^3 |
| %ind_r_0% | density at previous time step |
| %ind_r_AddDispPh% | |
| %ind_r_c% | intermediate density computed after correction pressure computation [kg/m^3] |
| %ind_R_P% | partial derivative of density with respect to pressure [s^2/m^2] |
| %ind_r_pDyn% | intermediate density, computed after dynamic pressure computation |
| %ind_r_sm% | smoothed density, unit kg/m^3 |
| %ind_Sexx% | Elastic solid stress tensor xx-component [Pa] |
| %ind_Sexy% | Elastic solid stress tensor xy-component [Pa] |
| %ind_Sexz% | Elastic solid stress tensor xz-component [Pa] |
| %ind_Seyy% | Elastic solid stress tensor yy-component [Pa] |
| %ind_Seyz% | Elastic solid stress tensor yz-component [Pa] |
| %ind_Sezz% | Elastic solid stress tensor zz-component [Pa] |
| %ind_SIG% | surface tension, unit: N/m |
| %ind_SlidingState% | |
| %ind_Smises% | vonMises-norm of solid stress tensor [Pa] |
| %ind_Sn(1)% | Stress tensor times boundary normal, i.e. stresses acting on surface, unit=Pa |
| %ind_Sn(2)% | Stress tensor times boundary normal, i.e. stresses acting on surface, unit=Pa |
| %ind_Sn(3)% | Stress tensor times boundary normal, i.e. stresses acting on surface, unit=Pa |
| %ind_SrelaxTime% | |
| %ind_Sxx% | solid stress tensor xx-component [Pa] |
| %ind_Sxy% | solid stress tensor xy-component [Pa] |
| %ind_Sxz% | solid stress tensor xz-component [Pa] |
| %ind_Syy% | solid stress tensor yy-component [Pa] |
| %ind_Syz% | solid stress tensor yz-component [Pa] |
| %ind_Szz% | solid stress tensor zz-component [Pa] |
| %ind_T% | Temperature, unit: Kelvin, Celsius |
| %ind_T_0% | temperature [K, °C] at previous time step |
| %ind_tauW% | effective turbulent wall shear stress [N/m^2] in direction of motion |
| %ind_tauWv(1)% | x-component of turbulent wall shear stress [N/m^2] |
| %ind_tauWv(2)% | y-component of turbulent wall shear stress [N/m^2] |
| %ind_tauWv(3)% | z-component of turbulent wall shear stress [N/m^2] |
| %ind_TurbulentWallLayer% | distance of artificial shift of MESHFREE points at boundary towards the interior if turbulence model is switched on |
| %ind_v(1)% | x-component of velocity vector |
| %ind_v(2)% | y-component of velocity vector |
| %ind_v(3)% | z-component of velocity vector |
| %ind_v0Darcy(1)% | velocity of the porous basis material, x-component, unit: m/s |
| %ind_v0Darcy(2)% | velocity of the porous basis material, y-component, unit: m/s |
| %ind_v0Darcy(3)% | velocity of the porous basis material, z-component, unit: m/s |
| %ind_v_0(1)% | velocity of the previous time step, x-component |
| %ind_v_0(2)% | velocity of the previous time step, y-component |
| %ind_v_0(3)% | velocity of the previous time step, z-component |
| %ind_v_3d(1)% | |
| %ind_v_3d(2)% | |
| %ind_v_3d(3)% | |
| %ind_v_tild(1)% | velocity before correction, x-component |
| %ind_v_tild(2)% | velocity before correction, y-component |
| %ind_v_tild(3)% | velocity before correction, z-component |
| %ind_v_times_v0% | scalar product (v-v_p)*(v0-v_p) |
| %ind_vn_a% | |
| %ind_vn_b% | |
| %ind_vn_n% | |
| %ind_vrel(1)% | |
| %ind_vrel(2)% | |
| %ind_vrel(3)% |