VMFL022
VMFL022
Cavitation
Over a Sharp-Edged Orifice Case B: Low Inlet Pressure
Overview
| Reference | W.H. Nurick, “Orifice Cavitation and Its Effects on Spray Mixing”, Journal of Fluids Engineering, Vol 98, pp. 681-687, 1976 | |
| Solver | Ansys Fluent | |
| Physics/Models | Turbulent multiphase flow with cavitation and phase change | |
| Input File |
| |
| Project Files | Link to Project Files Download Page |
Test Case
A steady, axisymmetric, multiphase (water/steam) flow, with phase change taking place. Due to sudden contraction a low pressure region occurs near the sharp edge which results in a weak cavitation. Figure 59: Flow Domain depicts the orifice geometry. Flow direction is from left to right.
| Material Properties | Geometry | Boundary Conditions |
|---|---|---|
|
Liquid: Water Density: 1000 kg/m3 Viscosity: 0.001 kg/m-s Gas: Water-Vapor Density: 0.02558 kg/m3 Viscosity: 1.26x10-6 kg/m-s |
L1 = 1.60 cm L2 = 3.20 cm r1 = 1.15 cm r2 = 0.40 cm |
P1 = 250,000 Pa P2 = 95,000 Pa T = 300 K Pvapor = 3,540 Pa |
Analysis Assumptions and Modeling Notes
The flow is steady and incompressible. Pressure based solver is used. Standard k-ε model with standard wall functions is used for turbulence. The Zwart-Gerber-Belamri cavitation model is applied together with mixture multiphase model.
For analysis of results, we calculate and compare the discharge coefficient with the experimental data.
The coefficient of discharge, 
,
is the ratio of the mass flow rate through the nozzle to the theoretical
maximum mass flow rate:
In the above equation, 
is the mass flow rate as calculated
by the CFD solver.
