Theory
The density and the characteristic impedance scale with the pressure; the speed of sound and the dynamic viscosity do not, so the kinematic viscosity falls as the pressure rises. A pressurised gas therefore has thinner viscous boundary layers in small holes: the perforate constant of a micro-perforated plate rises with the pressure. The panel states the factor by which of the same hole at the same frequency differs from dry air at 1 atm and 20 °C.
Equations
| where | meaning | unit |
|---|---|---|
| Density | kg/m³ | |
| Operating static pressure | Pa | |
| Molar mass of the gas | kg/kmol | |
| Universal gas constant, 8314.47 | J/(kmol K) | |
| Gas temperature | K | |
| Speed of sound | m/s | |
| Ratio of specific heats at | - | |
| Kinematic viscosity | m²/s | |
| Dynamic viscosity (Sutherland) | Pa s |
| where | meaning | unit |
|---|---|---|
| Ratio of the perforate constant to its value in dry air at 1 atm, 20 °C | - | |
| Kinematic viscosity of dry air at 1 atm, 20 °C | m²/s |
Default and rule
- Default
- ambient pressure + gauge pressure
- Rule
Computed from the ambient pressure and the gauge pressure.
- Source
The ideal-gas relations of the program's gas model.
Valid range at least 20 kPa
Typed or read-only
It can be typed only when the flow is not solved; then the gauge value is stored.