The method of equivalent networks was originally designed for a sequence of layers without constrictions. The impedance at a layer boundary is defined by the ratio of sound pressure p and normal velocity v, both averaged over the boundary surface S, \(Z={\langle p\rangle _{S}}/{\langle v\rangle _{S}}\). A layer with constrictions (e.g. a plate with the neck of a resonator) can be included in the equivalent network scheme if an orifice partition impedance (or simply: orifice impedance) Z\({}_{{M}}\) is added to the orifice of the constriction. This is a partition impedance of the type \(Z_{p}={\langle\Delta p\rangle _{S}}/{\langle v\rangle _{S}}\) with \(\Delta p=(p_{{front}}-p_{{back}})\) the sound pressure drop across the plane of the orifice and v the particle velocity through the orifice (in the direction front\(\to\)back).
Assume the area of the orifice is s (e.g. \(s=\) the cross-section area of a neck) with the porosity \(\sigma=s/S\) (e.g. \(S=\)cross-section area of a single...
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Mechel, F.P.: Schallabsorber, Vol. II, Ch. 2: Equivalent networks. Hirzel, Stuttgart (1995)
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© 2008 Springer-Verlag
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(2008). Partition Impedance of Orifices. In: Mechel, F.P. (eds) Formulas of Acoustics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-540-76833-3_47
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DOI: https://doi.org/10.1007/978-3-540-76833-3_47
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