SpectraSim Documentation
Parameter · 05 Boundary Conditions

Hole diameter (acoustics)

perforate.hole_diameter Unit: mm Step 05 · Boundary Conditions

The diameter of one hole of the perforated wall, as used by the acoustic impedance model. It sets the viscous resistance of the hole, its end corrections and, on auto, the discharge coefficient.

Last updated

Theory

The acoustic impedance of a perforate is computed per hole (Acoustic impedance model of a perforated wall). The hole diameter dd enters every model:

  • the viscous boundary layer in the hole scales with the radius a=d/2a = d/2 (the Stokes number ksak_s a, equation (1));
  • the inertia of the air in and around the hole grows with the end correction, a multiple of dd, equation (3);
  • the Elnady model adds a resistive end correction that is a cubic in dd, equation (2), and its radiation resistance depends on kdkd.

In a CFD + acoustics case with a perforated tube (or a thick plate), the hole diameter is entered once on the flow part of the card (Hole diameter) and the acoustic field is hidden; both use the same stored value.

The diameter also selects the auto discharge coefficient (Discharge coefficient C_D (acoustics)) through the d×td \times t table.

Equations

ksa=−iωρ/μ  d2k_s a = \sqrt{-i\omega\rho/\mu}\;\frac{d}{2}
(1)
δre=0.2 d+200 d2+16000 d3(d in m)\delta_{re} = 0.2\,d + 200\,d^2 + 16000\,d^3 \quad (d\ \text{in m})
(2)
end correction=ϵ d  (thin plate, ϵ=0.85),0.75 d  (Sullivan & Crocker, cross-flow),0.5 d fint  (Elnady, reactive)\text{end correction} = \epsilon\,d\ \ (\text{thin plate, } \epsilon = 0.85), \qquad 0.75\,d\ \ (\text{Sullivan \& Crocker, cross-flow}), \qquad 0.5\,d\,f_{int}\ \ (\text{Elnady, reactive})
(3)
wheremeaningunit
ddHole diameterm
aaHole radiusm
ω\omegaAngular frequencyrad/s
ρ,μ\rho, \muDensity and dynamic viscosity of the gaskg/m³, Pa s
δre\delta_{re}Resistive end correction of the Elnady modelm
ϵ\epsilonEnd-correction factor-
fintf_{int}Hole-interaction factor-

Default and rule

Default
3.0 mm shown on a new wall (the case file stores none until the card is saved)
Rule

The card shows 3.0 mm for a wall that has no hole diameter yet; the value is stored when the card is saved. There is no automatic estimate: enter the real diameter of the holes. The value is stored in m and shown in mm.

Source

Resistive end correction and the other Elnady terms: (Elnady et al., 2010). Measured ranges of the models: (Lee and Ih, 2003), (Kirby and Cummings, 1998), (Sullivan and Crocker, 1978).

Valid range > 0; each impedance model has its own measured range (see Range)

Model ranges

Elnady's CDC_D table was measured for d 0.6-2.4 mm (values up to 5 mm are extrapolated; beyond that the edge value is used); Lee & Ih 2-9 mm; Sullivan & Crocker measured one plate with d 2.49 mm.

Outside the range

The acoustic QA gate lists a diameter outside the selected model's range as a warning; the run continues.

References 4

  1. Elnady, T., Åbom, M. and Allam, S. (2010). Modeling perforates in mufflers using two-ports. Journal of Vibration and Acoustics, 132(6), 061010. DOI 10.1115/1.4001510
  2. Kirby, R. and Cummings, A. (1998). The impedance of perforated plates subjected to grazing gas flow and backed by porous media. Journal of Sound and Vibration, 217(4), 619-636. DOI 10.1006/jsvi.1998.1811
  3. Lee, S.-H. and Ih, J.-G. (2003). Empirical model of the acoustic impedance of a circular orifice in grazing mean flow. The Journal of the Acoustical Society of America, 114(1), 98-113. DOI 10.1121/1.1581280
  4. Sullivan, J. W. and Crocker, M. J. (1978). Analysis of concentric-tube resonators having unpartitioned cavities. The Journal of the Acoustical Society of America, 64(1), 207-215. DOI 10.1121/1.381963