“…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])
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).…”