Theory
The wall itself is not meshed with a thickness: it is a zero-thickness cyclic pair of faces. The thickness enters in three places:
- The jump's length: OpenFOAM's
porousBafflePressuremultiplies its per-length coefficients by a length (OpenFOAM user guide, 2026); the program writes and length , so the inertial loss is independent of , equation (1). The viscous Darcy term (Darcy coefficient D) does scale with . - The thick-plate formula of a perpendicular plate: (Plate formula).
- The no-grazing discharge coefficient of a perforated tube, interpolated in a table of hole diameter and thickness (Discharge coefficient C_D0). The thickness also feeds the acoustic perforate models.
Equations
| where | meaning | unit |
|---|---|---|
| Pressure jump | Pa | |
| Wall thickness | m | |
| Dynamic viscosity | Pa·s | |
| Darcy coefficient | 1/m² | |
| Loss coefficient | - | |
| Velocity normal to the wall face | m/s |
Default and rule
- Default
- 1 mm
- Rule
1 mm.
- Source
Jump law: (OpenFOAM user guide, 2026). Thick plate: (Idelchik, 2008). Discharge-coefficient table: Elnady's measured values (doctoral thesis, KTH 2004; the related paper is (Elnady et al., 2010)).
Valid range t > 0
Values
Above 0, in millimetres on the card.
Thickness and K
A typed is not corrected for the thickness; the thin-plate formula ignores it. Use the thick-plate formula or a measured for a sheet that is thick relative to its holes.
Outside the discharge-coefficient table
The table covers 0.5-2.5 mm; outside it the edge value is used (the card says so). Elnady measured 0.8-2.4 mm; the rest of the table is his extrapolation.
Related 5
References 3
- Elnady, T., Åbom, M. and Allam, S. (2010). Modeling perforates in mufflers using two-ports. Journal of Vibration and Acoustics, 132(6), 061010. DOI 10.1115/1.4001510
- Idelchik, I. E. (2008). Handbook of Hydraulic Resistance, 4th edition revised and augmented. Begell House. DOI 10.1615/978-1-56700-251-5.0
- OpenCFD Ltd. (2026). OpenFOAM user guide. openfoam.com. Web page