Theory
The empirical equivalent-fluid models write the characteristic impedance and propagation constant of a fibrous packing as power laws in one variable, equations (1)-(2). Delany and Bazley (Delany and Bazley, 1970) and Miki (Miki, 1990) used , which the program writes with the gas density as (dimensionless); Komatsu (Komatsu, 2008) used with in m³/kg, a variable without the gas density. Select the form in which the user constants User constant C1 ... C8 were fitted. With the Komatsu form the constants of a power law in a variable that falls with frequency have negative exponents (Komatsu: , ).
Equations
| where | meaning | unit |
|---|---|---|
| Model variable (this setting) | - | |
| Density and sound speed of the gas in the packing | kg/m³, m/s | |
| Frequency | Hz | |
| Flow resistivity at the local temperature | Pa·s/m² | |
| User constants | - |
Default and rule
- Default
- ρ₀ f / R (Delany-Bazley, Miki form)
- Rule
.
- Source
The two forms are those of the program's built-in models, as given by Komatsu Komatsu (2008).
Valid range ρ₀ f / R | 2 − log₁₀(f / R)
No validity check
A user-defined model has no known validity range; the acoustic QA gate does not flag any frequency.
Komatsu form
becomes 0 or negative for m³/kg, where a non-integer power is undefined; keep the sweep and resistivity inside the range of your fit.
Related 4
References 3
- Delany, M. E. and Bazley, E. N. (1970). Acoustical properties of fibrous absorbent materials. Applied Acoustics, 3(2), 105-116. DOI 10.1016/0003-682X(70)90031-9
- Komatsu, T. (2008). Improvement of the Delany-Bazley and Miki models for fibrous sound-absorbing materials. Acoustical Science and Technology, 29(2), 121-129. DOI 10.1250/ast.29.121
- Miki, Y. (1990). Acoustical properties of porous materials: modifications of Delany-Bazley models. Journal of the Acoustical Society of Japan (E), 11(1), 19-24. DOI 10.1250/ast.11.19