2008
DOI: 10.1016/j.apacoust.2007.02.004
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Influence of wall absorption on low-frequency dependence of reverberation time in room of irregular shape

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Cited by 31 publications
(19 citation statements)
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“…However, in the low-frequency limit typical materials covering room walls are characterized by a low absorption: ℜe(Z)/ρc ≫ 1, thus it is possible to assume that the shapes of modes are well approximated by the uncoupled eigenfunctions Φ n determined for hard room walls (Dowell et al, 1977). Taking all this into account and assuming that a source term in the wave equation has the form −q(r) cos(ωt), where q(r) and ω are the volume source distribution and the source frequency, the sound pressure in a steady-state can be determined by (Meissner, 2008a) …”
Section: Room Acoustics In Low-frequency Rangementioning
confidence: 99%
“…However, in the low-frequency limit typical materials covering room walls are characterized by a low absorption: ℜe(Z)/ρc ≫ 1, thus it is possible to assume that the shapes of modes are well approximated by the uncoupled eigenfunctions Φ n determined for hard room walls (Dowell et al, 1977). Taking all this into account and assuming that a source term in the wave equation has the form −q(r) cos(ωt), where q(r) and ω are the volume source distribution and the source frequency, the sound pressure in a steady-state can be determined by (Meissner, 2008a) …”
Section: Room Acoustics In Low-frequency Rangementioning
confidence: 99%
“…In low-frequency range, the reverberant behaviour of room is strongly frequency dependent (Meissner, 2007b(Meissner, , 2008b. Thus, in a theoretical model it was assumed that a room is excited by a a pure-tone sound source.…”
Section: Simulation Of Reverberant Response Of Roommentioning
confidence: 99%
“…When a steady-state is achieved, the source is abruptly switched off and the sound energy accumulated inside the room interior is absorbed on walls and an acoustic reverberation takes place. This reverberation consists of carrier waveforms of the decaying envelope that can be described by exponentially decreasing cosinusoidal functions (Meissner, 2008b)…”
Section: Simulation Of Reverberant Response Of Roommentioning
confidence: 99%
“…In this case the function describing time behaviour of the first mode (m, n = 0), the so-called Helmholtz mode that has an eigenfrequency equal to zero, is described by [24] P 00 (t) = Q 00 exp(−2r 00 t) ω 2 + 4r 2 00…”
Section: Theorymentioning
confidence: 99%