Fundamentals and Applications of Acoustic Metamaterials 2019
DOI: 10.1002/9781119649182.ch3
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Slow Sound and Critical Coupling to Design Deep Subwavelength Acoustic Metamaterials for Perfect Absorption and Efficient Diffusion

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Cited by 5 publications
(7 citation statements)
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“…Following the e iω t convention (ω = 2π f is the angular frequency), ζ Rad for a baffled circular open duct can be explicitly written as (see, for example, page 186 of [45]) ζRadbadbreak=[pz0u]Open endgoodbreak=1goodbreak−J1false(2k0RDfalse)k0RDgoodbreak+normaliSH1false(2k0RDfalse)k0RD\[{\zeta _{{\rm{Rad}}}} = {\left[ {\frac{p}{{{z_0}u}}} \right]_{{\rm{Open}}\;{\rm{end}}}} = 1 - \frac{{{J_1}(2{k_0}{R_{\rm{D}}})}}{{{k_0}{R_{\rm{D}}}}} + {\rm{i}}\frac{{S{H_1}(2{k_0}{R_{\rm{D}}})}}{{{k_0}{R_{\rm{D}}}}}\] where J 1 is the first‐order Bessel function of the first kind, SH 1 denotes the first‐order Struve‐H function, and k 0 = ω/ c 0 is the acoustic wavenumber. By using the transfer matrix method, [ 34,35 ] the reflection and transmission coefficients R and T in Equations (2) and thus the absorption coefficient α in Equation (1) can be explicitly expressed as functions of the radiation impedance ζ Rad (i.e., a known function of frequency) as well as the structural parameters of the Helmholtz resonators. Specifically, the acoustic response of each resonator is fully determined by 6 structural parameters: the radius R N and thickness T N of the neck, the depth H C , axial width L x , and circular angle θ C of the cavity, as well as the axial position x HR of the resonator (see Figure 1).…”
Section: General Methodology Of the Designmentioning
confidence: 99%
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“…Following the e iω t convention (ω = 2π f is the angular frequency), ζ Rad for a baffled circular open duct can be explicitly written as (see, for example, page 186 of [45]) ζRadbadbreak=[pz0u]Open endgoodbreak=1goodbreak−J1false(2k0RDfalse)k0RDgoodbreak+normaliSH1false(2k0RDfalse)k0RD\[{\zeta _{{\rm{Rad}}}} = {\left[ {\frac{p}{{{z_0}u}}} \right]_{{\rm{Open}}\;{\rm{end}}}} = 1 - \frac{{{J_1}(2{k_0}{R_{\rm{D}}})}}{{{k_0}{R_{\rm{D}}}}} + {\rm{i}}\frac{{S{H_1}(2{k_0}{R_{\rm{D}}})}}{{{k_0}{R_{\rm{D}}}}}\] where J 1 is the first‐order Bessel function of the first kind, SH 1 denotes the first‐order Struve‐H function, and k 0 = ω/ c 0 is the acoustic wavenumber. By using the transfer matrix method, [ 34,35 ] the reflection and transmission coefficients R and T in Equations (2) and thus the absorption coefficient α in Equation (1) can be explicitly expressed as functions of the radiation impedance ζ Rad (i.e., a known function of frequency) as well as the structural parameters of the Helmholtz resonators. Specifically, the acoustic response of each resonator is fully determined by 6 structural parameters: the radius R N and thickness T N of the neck, the depth H C , axial width L x , and circular angle θ C of the cavity, as well as the axial position x HR of the resonator (see Figure 1).…”
Section: General Methodology Of the Designmentioning
confidence: 99%
“…where J 1 is the first-order Bessel function of the first kind, SH 1 denotes the first-order Struve-H function, and k 0 = ω/c 0 is the acoustic wavenumber. By using the transfer matrix method, [34,35] the reflection and transmission coefficients R and T in Equations ( 2) and thus the absorption coefficient α in Equation (1) can be explicitly expressed as functions of the radiation impedance ζ Rad (i.e., a known function of frequency) as well as the structural parameters of the Helmholtz resonators. Specifically, the acoustic response of each resonator is fully determined by 6 structural parameters: the radius R N and thickness T N of the neck, the depth H C , axial width L x , and circular angle θ C of the cavity, as well as the axial position x HR of the resonator (see Figure 1).…”
Section: General Methodology Of the Designmentioning
confidence: 99%
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“…These solutions may further benefit from the use of (i) phononic crystals (PCs) and (ii) periodic MMs, since these may possess phononic band gaps, i.e. frequency ranges where no free wave propagation is allowed in the solid medium [17]. Such frequency bands arise typically due to the mechanisms of (i) Bragg scattering [18], in which case the frequency range is associated with the periodicity of the medium, and (ii) local resonance [19], where Fano-like interference is capable of opening band gaps in the sub-wavelength scale [20].…”
Section: Introductionmentioning
confidence: 99%
“…Meanwhile, the underwater good sound absorption of meta-structures has been proved by experiments (4-20 kHz) 18) and applications. 19) Inspired by airborne meta-structures, to overcome the high bulk modulus and low viscosity of water, underwater metastructures based on local resonance units have been used to absorb acoustic waves; 17,[20][21][22][23][24][25][26][27][28] most of these structures have performed poorly in terms of thickness and broadband sound absorption at low frequencies. Clearly, the difficulty of developing underwater meta-structures is related to the absorption of low-frequency broadband acoustic waves.…”
mentioning
confidence: 99%