Theory
Rogers and Hersh define the grazing velocity as the free-stream velocity past the orifice, outside the wall boundary layer (Rogers and Hersh, 1975). The velocity ON the perforated wall is not that: the cyclic baffle face averages the fast tube side with the slow chamber side, which would lower and therefore .
With "CFD, tube core":
- At each evaluation the solver writes two extra velocity samples, at a distance from the wall along each side's own face normal (equation 1): one inside the tube and one in the chamber.
- Each wall face takes the tangential speed of the nearest sample point on each side, and the faster side is used as , equation (2).
- The tube radius comes from a cylinder fit to the exported wall surface; when the wall is not tube-shaped, mm.
- If the core samples are missing, the wall's own tangential velocity is used and the K record says so (the grazing speed, and therefore , is then low).
With "Mach number", is the typed Mach number times the speed of sound at the material temperature, the same for every face.
Equations
| where | meaning | unit |
|---|---|---|
| Distance of the core samples from the wall | m | |
| Radius of the tube fitted to its surface | m | |
| Tangential speed at the sample of side a / b nearest to face | m/s | |
| Typed grazing Mach number | - | |
| Speed of sound at the material temperature | m/s |
Default and rule
- Default
- CFD, tube core
- Rule
CFD, tube core.
- Source
The definition of : (Rogers and Hersh, 1975). The core sampling is the program's way of obtaining that free-stream velocity, because the face value on the baffle includes the slow chamber side. Sampling uses OpenFOAM's
surfacesfunction object (patchInternalField,offsetMode normal) (OpenFOAM user guide, 2026).
Valid range CFD, tube core | Mach number
When to use Mach
When the solved core flow is not representative (for example a check of the model at a known grazing speed), or for a quick comparison.
Mach and temperature
The Mach option uses the speed of sound at the Material step's temperature, not the local gas temperature of a compressible run.