Soundproof structure body
US-2020234687-A1 · Jul 23, 2020 · US
US11636839B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11636839-B2 |
| Application number | US-202017039072-A |
| Country | US |
| Kind code | B2 |
| Filing date | Sep 30, 2020 |
| Priority date | Apr 18, 2018 |
| Publication date | Apr 25, 2023 |
| Grant date | Apr 25, 2023 |
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Provided is a soundproof structure body including an opening member that forms an opening tube line having a cross-sectional area S, and at least two resonance structures for sound waves that are installed inside the opening tube line, and in a case where a cross-sectional area of the resonance structure is defined as Si, a width thereof is defined as di, an interval between the two resonance structures is defined as L, an impedance of the two resonance structures is defined as Zi, and a synthetic acoustic impedance is defined as Zc, a condition of Expression (1) is satisfied at a resonance frequency f0 at which a theoretical absorption value At is a maximum value. This soundproof structure body can realize high absorption using a plurality of resonance structures.At(f0, L, S, Si, di, Zi)>0.75 (1),Here, L>0, S>0, Si (i=1, 2)>0, di (i=1, 2)>0
Opening claim text (preview).
What is claimed is: 1. A soundproof structure body comprising: an opening member that forms an opening tube line having a cross-sectional area S; and at least two resonance structures for sound waves that are installed inside the opening tube line, wherein a cross-sectional area Si (i=1, 2, . . . , where the resonance structure having a smaller i number is located on an upstream side) in the opening tube line and a width di (i=1, 2, . . . ) of the resonance structure in a waveguide forward direction are more than 0, at least two resonance structures among the resonance structures are installed to be spaced apart at an interval L (L>0) from each other, and in a case where an impedance of each of the two resonance structures installed to be spaced apart at the interval L from each other is defined as Zi (i=1, 2), and a synthetic acoustic impedance, in which the two resonance structures and the interval thereof, a change in the cross-sectional area in the waveguide forward direction, and the two resonance structures are considered, is defined as Zc, a condition of Expression (1) is satisfied at a resonance frequency f0 at which a theoretical absorption value At given by Expression (2) is a maximum value, At ( f 0, L, S, Si, di, Zi )>0.75 (1), where, in a case where L>0, S>0, Si(i=1, 2)>0, di(i=1, 2)>0, and, f, L, S, Si, di, Zi (i=1, 2) is represented by x, At ( x )=1−|( Zc ( x )− Z 0)/( Zc ( x )+ Z 0)| 2 −|2/( Ac ( x )+ Bc ( x )/ Z 0+ Z 0 Cc ( x )+ Dc ( x ))| 2 (2), where, the synthetic acoustic impedance Zc(x) is defined by Expression (3) Zc ( x ) = Z 0 A C ( x ) + B C ( x ) Z 0 C C ( x ) + D C ( x ) , ( 3 ) in Expression (3), Z0 is an acoustic impedance of an opening tube line represented by Zair/S(=Z0) (S is a tube line cross-sectional area), Zair denotes an acoustic impedance of air and is given by Zair=ρc, ρ denotes a density of air, and c denotes a speed of sound, Ac(x), Bc(x), Cc(x), and Dc(x) are elements of a synthetic transfer matrix, and are defined by Expression (4), and in Expression (4), Tc is a synthetic transfer matrix of the two resonance structures T C = T d 1 / 2 T 1 T d 1 / 2 T L - d 1 / 2 - d 2 / 2
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