Low-frequency broadband quasi-periodic sound insulation structure with gradient change of impedance and thickness
A gradient change, quasi-periodic technology, applied in the direction of sounding equipment, instruments, etc., can solve the problem of limited effective bandwidth and attenuation, and achieve the effect of strong designability, simple manufacturing process and wide selection range
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Embodiment 1
[0031] combine figure 1 , the parameters of the low-frequency broadband quasi-periodic sound insulation structure with impedance and thickness gradient changes are: Z A1 =2.2×10 6 kg / m 2 / s, Z B1 =34×10 6 kg / m 2 / s, Δd=0.2cm, ΔZ A =2×10 5 kg / m 2 / s, ΔZ B =2.25×10 6 kg / m 2 / s. The impedances of the two homogeneous media used in traditional periodic structures are 2.2×10 6 kg / m 2 / s and 34×10 6 kg / m 2 / s, and the thickness of each layer of medium is 3cm. Both structures have a period number of 5 and a total thickness of 30 cm.
[0032] figure 2 Medium A in the quasi-periodic structure 1 、A 2 、A 3 、A 4 、A 5 The impedance change curve, image 3 Medium B in the quasi-periodic structure 1 , B 2 , B 3 , B 4 , B 5 The impedance change curve. Figure 4 It is the band gap comparison result of the traditional periodic structure and the low-frequency broadband quasi-periodic sound insulation structure with impedance and thickness gradient changes. It can be s...
Embodiment 2
[0034] combine figure 1 , the parameters of the low-frequency broadband quasi-periodic sound insulation structure with impedance and thickness gradient changes are: Z A1 =2.6×10 6 kg / m 2 / s, Z B1 =34×10 6 kg / m 2 / s, Δd=0.5cm, ΔZ A =3×10 5 kg / m 2 / s, ΔZ B =3×10 6 kg / m 2 / s. The impedances of the two homogeneous media used in traditional periodic structures are 2.6×10 6 kg / m 2 / s and 34×10 6 kg / m 2 / s, and the thickness of each layer of medium is 3cm. Both structures have a period number of 5 and a total thickness of 30 cm.
[0035] Figure 5 Medium A in the quasi-periodic structure 1 、A 2 、A 3 、A 4 、A 5 The impedance change curve, Figure 6 Medium B in the quasi-periodic structure 1 , B 2 , B 3 , B 4 , B 5 The impedance change curve. Figure 7 It is the band gap comparison result of the traditional periodic structure and the low-frequency broadband quasi-periodic sound insulation structure with impedance and thickness gradient changes. It can be see...
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