2022
DOI: 10.1016/j.jsv.2022.116784
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PID-like active impedance control for electroacoustic resonators to design tunable single-degree-of-freedom sound absorbers

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Cited by 10 publications
(6 citation statements)
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“…Such subwavelength acoustic control can theoretically be extended down to even lower frequencies, but limitations of the experimental setup prevent us from measuring lower frequencies with a sufficient signal-to-noise ratio. The highest considered frequency is limited due to several assumptions in the analytical model that do not hold anymore at high frequencies (in particular, the collocation of heat and force sources), and delays in the control system that lead to an unavoidable drift in the achieved impedance 25 , as well as the approximation of the control transfer function by rational polynomials of finite order. As a reference case, we also plot the absorption curve of a porous material of similar thickness backed by a hard wall.…”
Section: Resultsmentioning
confidence: 99%
“…Such subwavelength acoustic control can theoretically be extended down to even lower frequencies, but limitations of the experimental setup prevent us from measuring lower frequencies with a sufficient signal-to-noise ratio. The highest considered frequency is limited due to several assumptions in the analytical model that do not hold anymore at high frequencies (in particular, the collocation of heat and force sources), and delays in the control system that lead to an unavoidable drift in the achieved impedance 25 , as well as the approximation of the control transfer function by rational polynomials of finite order. As a reference case, we also plot the absorption curve of a porous material of similar thickness backed by a hard wall.…”
Section: Resultsmentioning
confidence: 99%
“…To better understand how the controls are implemented, we first describe the linear dynamics of the loudspeaker membrane in the time domain as follows: where v ( t ) and ξ ( t ) denote the axial inward velocity and displacement of the diaphragm, respectively. The resonance properties exhibited are related to the mechanical and electromagnetic parameters of the resonator actuated, namely the effective surface area and the moving mass of the diaphragm S d and M ms , the force factor of the moving coil B ℓ , the resistance factored into the global losses R ms , and the overall equivalent compliance C mc where both the elastic suspension of the loudspeaker and the compressibility of the fluid inside the enclosure are accounted for (details can be found in Rivet 38 or Guo et al 43 ).…”
Section: Methodsmentioning
confidence: 99%
“…Misestimations of these parameters can result in the synthesis of multiple-degreesof-freedom impedances, which is perhaps made evident by an increased evanescent component Im(q ) of the wave around the local resonance in the experimental dispersion. More-accurate impedance-synthesis control schemes may be worth investigating [40,41] to mitigate these effects. That being said, this high-energy dissipation at the resonance has little, if any, effect on the Bragg gap, which is the focus of this work.…”
Section: B Experimental Demonstrationmentioning
confidence: 99%