Theory
Lafarge et al. (Lafarge et al., 1997) introduced , the thermal analogue of the static viscous permeability , to describe the bulk modulus correctly at low frequency. In the bulk modulus of equation (1) it appears in the first term (low-frequency behaviour) and in the square root (the transition). With , JCAL reduces exactly to JCA; the program's tests confirm this.
Equations
| where | meaning | unit |
|---|---|---|
| Static thermal permeability (this setting) | m² | |
| Thermal characteristic length | m | |
| Porosity | - | |
| Gas: ratio of specific heats, absolute pressure, viscosity, Prandtl number, density | SI |
Default and rule
- Default
- blank = φ Λ'² / 8 (the JCA value)Computed by the program
- Rule
Blank: , so that JCAL behaves as JCA.
- Source
The JCAL model is that of Lafarge et al. (1997). Equation (1) follows an open reference description of the model and is implemented together with the JCA equations, which are cross-checked against Atalla and Panneton (2000). The 0.2-5 consistency band is the program's own check: a factor that catches a unit error, such as mm² entered for m².
Valid range > 0; warning outside 0.2-5 × φ Λ'² / 8
Values
Above 0, in m² (fibrous materials: of the order of m²).
Consistency
Outside 0.2-5 times the JCA value the QA gate warns: check the unit.
Verified
Checked in a full acoustic run of a packed resonator (2026-11-11): every quality check passes; with estimated parameters the TL agrees with Miki within about 1 dB below 1 kHz and falls 7-9 dB below it at 2 kHz.
Related 4
References 2
- Atalla, Y. and Panneton, R. (2000). Inverse characterization of the geometrical macroscopic parameters of porous materials. Canadian Acoustics, 28(3), 80-81. Web page
- Lafarge, D., Lemarinier, P., Allard, J. F. and Tarnow, V. (1997). Dynamic compressibility of air in porous structures at audible frequencies. The Journal of the Acoustical Society of America, 102(4), 1995-2006. DOI 10.1121/1.419690