SpectraSim Documentation
Parameter · 05 Boundary Conditions

Thermal characteristic length (JCA / JCAL)

thermal_length Unit: µm (stored in m) Step 05 · Boundary Conditions

A length that characterises the pore surface available for heat exchange between the gas and the fibres. It sets where the bulk modulus of the gas in the pores changes from isothermal (low frequency) to adiabatic (high frequency). It is an input of the JCA and JCAL models only; a blank field takes twice the viscous length.

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Theory

Champoux and Allard (Champoux and Allard, 1991) defined Λ′\Lambda' as twice the ratio of pore volume to pore surface. At low frequency the gas in the pores exchanges heat with the fibres and is compressed isothermally (bulk modulus P0/ϕP_0/\phi); at high frequency it is compressed adiabatically (γP0/ϕ\gamma P_0/\phi). The transition is controlled by the thermal length and, in JCAL, by the static thermal permeability, equation (1). In JCA, k0′k'_0 is not an input but follows from Λ′\Lambda', equation (2).

Equations

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}}
(1)
k0′=ϕΛ′28  (JCA; JCAL when its permeability is blank),Λ′=2Λ  (when blank)k'_0 = \frac{\phi\Lambda'^2}{8}\ \ \text{(JCA; JCAL when its permeability is blank)}, \qquad \Lambda' = 2\Lambda\ \ \text{(when blank)}
(2)
wheremeaningunit
Λ′\Lambda'Thermal characteristic length (this setting)m
Λ\LambdaViscous characteristic lengthm
k0′k'_0Static thermal permeabilitym²
KeqK_{eq}Equivalent bulk modulusPa
γ,P0,η,Pr,ρ0\gamma, P_0, \eta, \mathrm{Pr}, \rho_0Gas: ratio of specific heats, absolute pressure, viscosity, Prandtl number, densitySI
ϕ\phiPorosity-
ω\omegaAngular frequencyrad/s

Default and rule

Default
blank = 2 × viscous lengthComputed by the program
Rule

Blank: Λ′=2Λ\Lambda' = 2\Lambda, the usual ratio for fibrous materials.

Source

The equations are cross-checked against Atalla and Panneton (2000); the thermal length is defined by Champoux and Allard (1991). The ratio 2 is a common estimate for fibrous materials; it is not taken from a cited source.

Valid range > 0; ≥ viscous length

Values

Above 0; entered in µm.

Shorter than the viscous length

The QA gate warns when Λ′<Λ\Lambda' < \Lambda.

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 2

  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