The following table contains a list of variables (with both long and short variable names) that can be used when working with CFD calculations. For an explanation of the column headings, see List of Field Variables.
Note: Variables with names shown in bold text are not output to CFD-Post. However, some of these variables can be output to CFD-Post by selecting them from Extra Output Variables List on the Results tab of the Solver > Output Control details view of CFX-Pre.
Long Variable Name |
Short Variable Name |
Units |
Availability |
Definition |
---|---|---|---|---|
Density |
density |
[kg m^-3] ![]() |
1 A, C, M, P, R, TS |
Mass per unit volume. Note that for fixed composition,
variable composition, and reacting mixtures, when density is
governed by the
|
Dynamic Viscosity |
viscosity |
[kg m^-1 s^-1] |
2 A, C, M, P, R, TS |
Dynamic viscosity ( |
Velocity[a] |
vel |
[m s^-1] |
1 A, C, M, P, R, TS |
Velocity vector. |
Velocity u Velocity v Velocity w |
u v w |
[m s^-1] |
1 A, C, M, P, R, TS |
Components of velocity. |
Pressure |
p |
[kg m^-1 s^-2] |
1 A, C, M, P, R, TS |
Both |
Static Pressure |
pstat |
[kg m^-1 s^-2] |
3 |
CFX solves for the relative |
Total Pressure |
ptot |
[kg m^-1 s^-2] |
2 A, C, M, P, R, TS |
The total pressure, |
Wall Shear |
wall shear |
Pa |
3,B |
For details, see Scalable Wall Functions in the CFX-Solver Theory Guide. |
Volume of Finite Volume |
|
3 C, DT, R, TS |
Volume of finite volume. For details, see Discretization of the Governing Equations in the CFX-Solver Theory Guide. | |
X coordinate |
x |
[m] |
2 C | |
Y coordinate |
y |
[m] |
2 C | |
Z coordinate |
z |
[m] |
2 C | |
Kinematic Diffusivity |
visckin |
2 C, M, P, R, TS |
Kinematic diffusivity describes how rapidly a scalar quantity would move through the fluid in the absence of convection. For convection-dominated flows, the kinematic diffusivity can have little effect because convection processes dominate over diffusion processes. | |
Shear Strain Rate |
sstrnr |
[s^-1] |
2 A, C, M, R, TS |
For details see Non-Newtonian Flow in the CFX-Solver Modeling Guide. |
Specific Heat Capacity at Constant Pressure |
Cp |
[m^2 s^-2 K^-1] |
2 A, C, M, R, TS |
For details, see Specific Heat Capacity in the CFX-Solver Modeling Guide. |
Specific Heat Capacity at Constant Volume |
Cv |
[m^2 s^-2 K^-1] |
2 A, C, M, P, R, TS |
|
Thermal Conductivity |
cond |
[kg m s^-3 K^-1] |
2 A, C, M, R, TS |
Thermal conductivity, For details, see Thermal Conductivity in the CFX-Solver Modeling Guide. |
Temperature |
T |
[K] |
1 A, C, DT, M, P, R, TS |
The static
temperature, |
Total Temperature |
Ttot |
[K] |
1 A, C, M, P, R, TS |
The total temperature is derived from the concept of total enthalpy and is computed exactly the same way as static temperature, except that total enthalpy is used in the property relationships. For details, see Total Temperature in the CFX-Solver Theory Guide. |
Wall Heat Flux |
Qwall |
[W m^-2] |
2,B C, DT, R, TS |
A heat flux is specified across the wall boundary. A positive value indicates heat flux into the domain. For multiphase cases, when the bulk heat flux into both phases is set, this option is labeled Wall Heat Flux instead of Heat Flux. When set on a per fluid basis, this option is labelled Heat Flux. |
Wall Heat Transfer Coefficient |
htc |
[W m^-2 K^-1] |
2,B C, R, TS |
For details, see Heat Transfer Coefficient and Wall Heat Transfer Coefficient in the CFX-Solver Modeling Guide. |
Total Enthalpy |
htot |
[m^2 s^-2] |
A, C, M, R, TS |
For details, see Transport Equations in the CFX-Solver Theory Guide. |
Static Enthalpy |
enthalpy |
[m^2 s^-2] |
2 A, C, M, P, R, TS |
For details, see Static Enthalpy in the CFX-Solver Theory Guide. |
[a] When a
rotating frame of reference is used, all variables in the CFX-5
results file are relative to the rotating frame, unless specified
as a Stn Frame
variable.