Theory
Each port face carries its own transverse modes , obtained from a two-dimensional eigenproblem on the face mesh, equation (1); the plane wave is . A mode propagates above its cut-off frequency, equation (2), and decays exponentially along the duct below it (evanescent), equation (3).
- The port boundary condition is non-reflecting for every mode it includes: each included mode leaves the model without reflection.
- A mode that is NOT included but is excited near the port (by an area step or a tube end close to it) is reflected by the port as if the port were rigid for that mode.
- Keeping the first few evanescent modes removes most of this spurious reflection.
The program includes every mode with plus this number of further modes, in order of increasing . The evanescent wavenumber is taken on the decaying branch, so the additional modes are stable.
Equations
| where | meaning | unit |
|---|---|---|
| Transverse shape of port mode (unit mean square over the face) | - | |
| Transverse wavenumber of mode | 1/m | |
| Cut-off frequency of mode | Hz | |
| Axial wavenumber (time dependence ) | 1/m | |
| Speed of sound at the port | m/s |
Default and rule
- Default
- 1
- Rule
1 further mode per port.
- Source
Validation of the modal port:
- The modes of circular ports are checked against the zeros of (tolerance 0.5 %; measured 0.017 % on 30 mm pipes and 0.01-0.17 % on the ports of case V2, a two-inlet single-chamber muffler with internal inlet and outlet tubes).
- A straight duct transmits with and no mode coupling.
- The power-normalised scattering matrix of six propagating modes at 5 kHz is unitary and reciprocal to .
Valid range 0 to 3
Values
0 to 3. The mode table on this step lists the modes each port includes.