2019
DOI: 10.1016/j.jsv.2019.07.002
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Dynamics and sound radiation of a dielectric elastomer membrane

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Cited by 22 publications
(23 citation statements)
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“…Due to non‐negligible electrode resistivity, the electric field on some portions of the DE material (far from the connections with the power electronics) might result in being lower than the target static value, limiting the DE material capability to uniformly achieve large convertible energy densities. [ 63 ] Indicating with R s the sheet resistance of the compliant electrodes, the characteristic R – C time constant of the electrodes‐DE assembly is τnormale=RnormalsCDEG. In contrast with τ d , time constant τnormale depends on both the DEG system dimensions and the materials properties, and it is required to be as small as possible.…”
Section: Generalities On Degsmentioning
confidence: 99%
“…Due to non‐negligible electrode resistivity, the electric field on some portions of the DE material (far from the connections with the power electronics) might result in being lower than the target static value, limiting the DE material capability to uniformly achieve large convertible energy densities. [ 63 ] Indicating with R s the sheet resistance of the compliant electrodes, the characteristic R – C time constant of the electrodes‐DE assembly is τnormale=RnormalsCDEG. In contrast with τ d , time constant τnormale depends on both the DEG system dimensions and the materials properties, and it is required to be as small as possible.…”
Section: Generalities On Degsmentioning
confidence: 99%
“…For the aim of sound reproduction (e.g., playing an audio file), choosing a time-dependent component of the voltage proportional to the desired output pressure will at least result in harmonic distortions due to the quadratic form of the voltage. For this reasons, different strategies have been proposed to suitably pre-process the voltage input as function of the desired acoustic output, 5,8,9 as further discussed in Sect. 4.…”
Section: Electro-elastic Model Of the Diaphragm Dynamicsmentioning
confidence: 99%
“…The pressure field generated by the speaker is calculated from the local velocities of the DE diaphragm elements through a discretisation of the Rayleigh integral, which approximates the diaphragm surface as a distribution of acoustic monopoles. 9 In the following, we use a time-domain formulation for the Rayleigh integral, which accounts for the DE membrane curvature. 9,17 We consider a cone-DEA mounted on an infinite baffle and a receptor point on the device axis at a distance h r from the axis.…”
Section: Radiated Acoustic Pressure Modelmentioning
confidence: 99%
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