SpectraSim Documentation
Parameter · 05 Boundary Conditions

User constant C8

user_constants.C8 Step 05 · Boundary Conditions

The exponent of the imaginary part (reactance) of the characteristic impedance in the user-defined equivalent-fluid model of a packing. Used only when Acoustic (poroacoustic) model of the packing is "user defined"; it pairs with User constant C7.

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Theory

The user-defined model has the form of the empirical models of Delany and Bazley (Delany and Bazley, 1970), Miki (Miki, 1990) and Komatsu (Komatsu, 2008): the characteristic impedance ZcZ_c and the propagation constant kck_c of the packing are power laws in one variable XX (Variable X of the user constants), equations (1)-(2). C1…C4C_1 \dots C_4 belong to kck_c (C1C_1, C2C_2 its real part, C3C_3, C4C_4 its imaginary part), C5…C8C_5 \dots C_8 to ZcZ_c (C5C_5, C6C_6 real, C7C_7, C8C_8 imaginary). From ZcZ_c and kck_c the program forms the equivalent density and bulk modulus that the acoustic solver gives the packing's elements, equation (3).

C8 is the exponent of the imaginary part (reactance) of the characteristic impedance. It sets how the reactance C7X−C8C_7 X^{-C_8} grows as XX falls.

Equations

Zc=ρ0c0[1+C5X−C6−i C7X−C8]Z_c = \rho_0 c_0\left[1 + C_5 X^{-C_6} - i\,C_7 X^{-C_8}\right]
(1)
kc=ωc0[1+C1X−C2−i C3X−C4]k_c = \frac{\omega}{c_0}\left[1 + C_1 X^{-C_2} - i\,C_3 X^{-C_4}\right]
(2)
ρeq=Zckcω,Keq=ωZckc\rho_{eq} = \frac{Z_c k_c}{\omega}, \qquad K_{eq} = \frac{\omega Z_c}{k_c}
(3)
wheremeaningunit
C8C_8This constant-
ZcZ_cCharacteristic impedance of the packingPa·s/m
kck_cPropagation constant (time dependence e+iωte^{+i\omega t})1/m
XXρ0f/R\rho_0 f/R or 2−log⁡10(f/R)2 - \log_{10}(f/R)-
ρ0,c0\rho_0, c_0Density and sound speed of the gas in the packingkg/m³, m/s
ω\omegaAngular frequencyrad/s
ρeq,Keq\rho_{eq}, K_{eq}Equivalent density and bulk moduluskg/m³, Pa

Default and rule

Default
0.632 (Miki's value)
Rule

0.632: the user-defined set starts from Miki's constants. For comparison, C8 is 0.732 in Delany-Bazley and -4.1 in Komatsu (whose variable is 2−log⁡10(f/R)2 - \log_{10}(f/R)).

Source

The model form and the built-in constant sets agree with Komatsu Komatsu (2008), Tables 1-2 and eqs. (15)-(18). User constants come from a fit to the measured ZcZ_c and kck_c of the material.

Valid range any real number; no validity range is checked

No validity range

The validity range of a user fit is not known, so the acoustic QA gate checks no frequency band. Keep the sweep inside the range of XX over which the constants were fitted.

Physical behaviour

Constants that make the real part of ZcZ_c or the decay of kck_c negative describe a material that creates energy; the passivity gate of the acoustic run (outgoing power must not exceed the incident power) can then fail.

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