THREE DIMENSIONAL TURBULENT-INCOMPRESSIBLE
FLUID FLOW ANALYSIS OF A RANGER QCT CONTROL VALVE
Joseph W. Smith
DRD Technology Corporation
Tulsa, OK
Keith Black
Cashco, Inc.
Ellsworth, KS
ABSTRACT
Cashco, Inc., desired to determine whether or not a Computational Fluid Dynamic (CFD) model could accurately predict the fluid flow through a Ranger QCT Control Valve. The control valve itself was created by Cashco and modeled using Pro/ENGINEERÒ Revision 19 solid geometry. ANSYS Revision 5.4 was used to create the finite element mesh, apply loads, solve, and evaluate the results of the fluid analysis. Two result quantities were of primary interest to Cashco, the Flow Coefficient (Cv) and the Pressure Recovery Factor (FL). The results of the fluid analysis showed that ANSYS predicted the Flow Coefficient and Pressure Recovery Factor to within 10% and 2% of their experimental values, respectively.
NOMENCLATURE
Cv is the flow coefficient
FL is the pressure recovery factor.
P1 is the upstream pressure of the fluid, in PSI, measured one pipe diameter upstream of the valve.
P2 is the downstream pressure of the fluid, in PSI, measured ten pipe diameters downstream of the value.
Pvc is the pressure of the fluid at the vena contracta, in PSI.
Q is the fluid flow rate, in GPM.
Sg is the specific gravity of the fluid.
INTRODUCTION
The goal of this analysis was to determine if ANSYS could predict the pressure distribution of water flowing through a Ranger QCT Control valve (rotary globe). The geometry was provided to DRD in the form of Pro/ENGINEER part and assembly files. The fluid geometry was created by DRD Technology also using Pro/ENGINEER Revision 19. DRD created a technique whereby the fluid flow paths in the control valve were transformed into solid geometry. This technique involves exporting IGES files representing the assembly from Pro/ENGINEER and then importing those IGES files back into Pro/ENGINEER. Prior to importing the IGES files, a simple block representing the fluid is imported first. Then, each IGES file is subsequently imported as a cut that removes a segment of the fluid. The removed segments of the geometry are voids in the flow field that represent the solid parts. Once the fluid flow geometry was completed, an IGES file was exported from Pro/ENGINEER and then imported into ANSYSÒ . Figure 1 shows a cut-away view of the control valve.

The valve assembly itself was composed of solid parts. For
the fluid analysis, however, the solid parts are not required. It is the open
void between the solid parts that must be meshed for the fluid analysis.
Therefore, the assembly must be "inverted", whereby, the fluid void
becomes a solid volume and any solid parts in the flow become voids. The
analysis assumes the fluid flow was isothermal and steady state. The water
temperature was 60° F (values for density and
viscosity for the fluid were determined based on this temperature and assumed to
be constant).
ANALYSIS GEOMETRY CREATION
The following section outlines the procedure used to create the finite element model of the fluid flow environment. This procedure assumes the solid geometry was originally created in Pro/ENGINEER and the flow field will be meshed with tetrahedron shaped elements.
Geometry Setup (Pro/ENGINEER):
Geometry Creation (Pro/ENGINEER):
Once all of the IGES files have been imported into the new part, the remaining geometry is of the flow field.
Refer to Figure 2 for a visual description of the fluid flow geometry near the valve created in Pro/ENGINEER.

Volume Creation (ANSYS):
Finite Element Model Creation (ANSYS):
Once all the elements have been changed from SOLID45s to FLUID142s the finite element model is complete and ready for boundary condition application. The analyzed model contained approximately 377,000 elements, 71,000 nodes, and 425,000 DOF’s (degrees-of-freedom). This mesh also included refinement in the boundary layer.
Please examine Figure 3 for a graphical representation of the finite element mesh near the valve.

BOUNDARY CONDITIONS
All exterior surfaces (except the inflow and outflow
boundaries) of the fluid domain were assumed to have no-slip conditions
(velocity components in the x, y, and z directions defined as zero). The inflow
boundary x-direction component (direction of flow) of velocity was set at –79.64
in/s. This corresponds to a volumetric flow rate of 854 GPM given by Cashco
(based on a pipe inside diameter of 8 in). For the given fluid properties, the
Reynold's number is approximately 360,000. The y and z components of velocity on
the inflow boundary were set to zero. The pressure on the outflow boundary was
set to 0 PSI. This is the standard ANSYS/FLOTRAN outlet condition and assumes
the flow is leaving at atmospheric pressure (0 PSI gage pressure).
ANALYSIS ASSUMPTIONS
RESULTS
The values for CV and FL are calculated as follows and shown in Table 1 (the actual calculations are shown in the Appendix).

| ANSYS Determined Value | Cashco Experimental Value | Percent Error | |
| Flow Coefficient (Cv) | 321 | 291 | 9.3% |
| Pressure Recovery Factor | 0.866 | 0.85 | 1.8% |
Where the pressures P1 and P2 where taken at the near wall nodes, Q derived from the mass flow balance given in the ANSYS/FLOTRAN output file (.pfl), and Sg being defined by CASHCO. The pressure at the vena contracta was deduced by CASHCO based on results like those shown in Figure 4. Determining the location and aggregate value of the vena contracta is difficult and somewhat subjective, especially for devices with multiple flow paths. The technique used for this model was to use a path plot (like the path shown in Figure 4) to determine the change in pressure as the flow passed near the center of the flow streams. The pressure at the vena contracta is the lowest value of pressure downstream of where the flow is locally restricted by the valve plug. From this data, the pressure at the vena contracta was determined to be approximately –2.3 PSI (12.4 PSI absolute pressure). The method used for determining the location of the vena contracta is not necessarily valid for all valve types for any given set of flow conditions. However, it is considered to by an accurate estimation of the pressure at the vena contracta for the Ranger QCT Control Valve with the given flow conditions. It should be noted that the actual test data was based on the flow conditions being compared to choked flow conditions in order to determine the pressure recovery factor rather than by direct measure of the vena contracta pressure.
The normalized rate of change for the momentum variables ranged from 1.6e-3 to 3.5e-3, turbulence variables ranged from 3.3e-3 to 7.2e-3, and the pressure variable was 3.6e-3. Figures 5 and 6 show a cut view of the pressure and velocity of the water flowing through the valve.
![]() |
![]() |
![]() |
CONCLUSIONS
Based on the calculated flow coefficient and pressure recovery factor, ANSYS is shown to compare favorably to the experimental results. Due to the results of this analysis, CASHCO decided to license and implement ANSYS/FLOTRAN.
REFERENCES
APPENDIX
The determination of the flow coefficient (Cv) and the pressure recovery factor (FL) are as follows.
From ANSYS:
Q=848 GPM
P1=7.0 PSI
P2=0.026 PSI
Pvc=-2.3 PSI
Sg=1

![]()
