SpectraSim Documentation
Parameter · 05 Boundary Conditions

Porosity (JCA / JCAL)

The open porosity of the packing: the fraction of its volume occupied by connected gas. An input of the JCA and JCAL acoustic models only (shown when one of them is chosen).

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Theory

In the JCA and JCAL models (Johnson et al., 1987), (Champoux and Allard, 1991) the packing is an equivalent fluid whose density and bulk modulus are those of the gas in the pores divided by ϕ\phi (the macroscopic form, equations (1)-(2)). The porosity scales both: a lower porosity raises the effective density and stiffness and so the characteristic impedance of the packing. It also enters the estimate of the viscous characteristic length when Viscous characteristic length (JCA / JCAL) is left blank, equation (3), and the JCA value of the thermal permeability.

Fibrous packings (glass, rock, steel wool) have porosities of about 0.9-0.99; the empirical models of Acoustic (poroacoustic) model of the packing assume a value near 1 implicitly.

Equations

ρeq=α∞ρ0ϕ[1+R ϕiωρ0α∞1+i 4α∞2ηρ0ωR2Λ2ϕ2]\rho_{eq} = \frac{\alpha_\infty\rho_0}{\phi}\left[1 + \frac{R\,\phi}{i\omega\rho_0\alpha_\infty}\sqrt{1 + i\,\frac{4\alpha_\infty^2\eta\rho_0\omega}{R^2\Lambda^2\phi^2}}\right]
(1)
Keq=γP0/ϕγ−(γ−1)[1−i ϕ η/Prk0′ρ0ω1+i 4k0′2ρ0ω(η/Pr)Λ′2ϕ2]−1K_{eq} = \frac{\gamma P_0/\phi}{\gamma - (\gamma - 1)\left[1 - i\,\dfrac{\phi\,\eta/\mathrm{Pr}}{k'_0\rho_0\omega}\sqrt{1 + i\,\dfrac{4 k_0'^2\rho_0\omega}{(\eta/\mathrm{Pr})\Lambda'^2\phi^2}}\right]^{-1}}
(2)
Λ=8 η α∞R ϕ  (when blank),k0′=ϕΛ′28  (JCA)\Lambda = \sqrt{\frac{8\,\eta\,\alpha_\infty}{R\,\phi}}\ \ \text{(when blank)}, \qquad k'_0 = \frac{\phi\Lambda'^2}{8}\ \ \text{(JCA)}
(3)
wheremeaningunit
ϕ\phiOpen porosity (this setting)-
α∞\alpha_\inftyTortuosity-
RRFlow resistivity at the local temperaturePa·s/m²
Λ,Λ′\Lambda, \Lambda'Viscous and thermal characteristic lengthsm
k0′k'_0Static thermal permeabilitym²
ρ0,η,γ,P0,Pr\rho_0, \eta, \gamma, P_0, \mathrm{Pr}Density, viscosity, ratio of specific heats, absolute pressure and Prandtl number of the gasSI
ω\omegaAngular frequencyrad/s

Default and rule

Default
0.95
Rule

0.95, typical of a fibrous packing.

Source

The equations are the macroscopic JCA / JCAL form, consistent term by term with Atalla and Panneton (2000). The default is the program's choice of a typical value for a fibrous packing; it is not derived from measured porosities of muffler packings.

Valid range 0 < φ ≤ 1; warning below 0.7

Values

0<ϕ≤10 < \phi \le 1 (refused otherwise).

Low porosity

Below 0.7 the acoustic QA gate warns: low for a fibrous or foam packing.

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.

References 3

  1. Atalla, Y. and Panneton, R. (2000). Inverse characterization of the geometrical macroscopic parameters of porous materials. Canadian Acoustics, 28(3), 80-81. Web page
  2. Champoux, Y. and Allard, J.-F. (1991). Dynamic tortuosity and bulk modulus in air-saturated porous media. Journal of Applied Physics, 70(4), 1975-1979. DOI 10.1063/1.349482
  3. Johnson, D. L., Koplik, J. and Dashen, R. (1987). Theory of dynamic permeability and tortuosity in fluid-saturated porous media. Journal of Fluid Mechanics, 176, 379-402. DOI 10.1017/S0022112087000727