SpectraSim Documentation
Parameter · 05 Boundary Conditions

Fibre type

Selects the measured data set used by the bulk-density estimate of the flow resistivity: glass wool or rock (basalt) wool. Used only when Resistivity input is "bulk density".

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Theory

Glass and rock wools of the same bulk density differ in fibre diameter, so their flow resistivities differ. The program uses a separate power law fitted to the measurements of each material in Komatsu (2008) (Table 3: 15 glass wools, 9 rock wools). At 30 kg/m³ the glass-wool fit gives about 1.2×10⁴ Pa·s/m² and the rock-wool fit about 1.1×10⁴; at 90 kg/m³, about 5.6×10⁴ and 6.2×10⁴.

Equations

R=A ρb B,(A,B)={(93.8, 1.420)glass wool(53.1, 1.571)rock woolR = A\,\rho_b^{\,B}, \qquad (A, B) = \begin{cases} (93.8,\ 1.420) & \text{glass wool} \\ (53.1,\ 1.571) & \text{rock wool} \end{cases}
(1)
wheremeaningunit
RREstimated flow resistivityPa·s/m²
ρb\rho_bBulk densitykg/m³

Default and rule

Default
glass wool
Rule

Glass wool.

Source

Power-law fits by the program to the measurements in Table 3 of Komatsu (2008).

Valid range glass wool | rock wool

Other materials

Only glass and rock wool are covered. For steel wool, ceramic fibre or foams, enter a measured flow resistivity instead.

References 1

  1. 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