SpectraSim Documentation
Parameter · 05 Boundary Conditions

Variable X of the user constants

The dimensionless variable in which the user-defined packing model's power laws are written: either ρ0f/R\rho_0 f/R (the Delany-Bazley and Miki form) or 2−log⁡10(f/R)2 - \log_{10}(f/R) (the Komatsu form). Used only when Acoustic (poroacoustic) model of the packing is "user defined".

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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 f/σf/\sigma, which the program writes with the gas density as X=ρ0f/RX = \rho_0 f/R (dimensionless); Komatsu (Komatsu, 2008) used 2−log⁡10(f/R)2 - \log_{10}(f/R) with f/Rf/R 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: C2=C6=−6.2C_2 = C_6 = -6.2, C4=C8=−4.1C_4 = C_8 = -4.1).

Equations

Zc=ρ0c0[1+C5X−C6−i C7X−C8],kc=ωc0[1+C1X−C2−i C3X−C4]Z_c = \rho_0 c_0\left[1 + C_5 X^{-C_6} - i\,C_7 X^{-C_8}\right], \qquad k_c = \frac{\omega}{c_0}\left[1 + C_1 X^{-C_2} - i\,C_3 X^{-C_4}\right]
(1)
X=ρ0fRorX=2−log⁡10fRX = \frac{\rho_0 f}{R} \qquad \text{or} \qquad X = 2 - \log_{10}\frac{f}{R}
(2)
wheremeaningunit
XXModel variable (this setting)-
ρ0,c0\rho_0, c_0Density and sound speed of the gas in the packingkg/m³, m/s
ffFrequencyHz
RRFlow resistivity at the local temperaturePa·s/m²
C1…C8C_1 \dots C_8User constants-

Default and rule

Default
ρ₀ f / R (Delany-Bazley, Miki form)
Rule

ρ0f/R\rho_0 f/R.

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

X=2−log⁡10(f/R)X = 2 - \log_{10}(f/R) becomes 0 or negative for f/R≥100f/R \ge 100 m³/kg, where a non-integer power is undefined; keep the sweep and resistivity inside the range of your fit.

References 3

  1. 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
  2. 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
  3. 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