2018
DOI: 10.1515/teme-2018-0066
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An inverse approach to the characterisation of material parameters of piezoelectric discs with triple-ring-electrodes

Abstract: For its usage in simulation-based design processes a precise knowledge of the employed material properties is inevitable. In the case of piezoelectric ceramics, the provided material parameters often suffer from large uncertainties and even inconsistencies since the standardised measurement procedure needs several specimens to determine a single set of material parameters. In contrast, the presented measurement set-up allows to calculate material parameters using one unique disc-shaped specimen with an optimis… Show more

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Cited by 2 publications
(3 citation statements)
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“…Setting F i = −v i Z m,i , this enables to solve equation ( 4) for the frequency-dependent electrical impedance Z el = u/i of the transducer model. In an inverse procedure, the parameters of the Mason model for a given ultrasonic transducer are identified by comparing the electrical impedance of the model Z el with the electrical impedance Z meas of a physical transducer [4]. As the physical transducer is to be used in an acoustic absorption measurement system based on an established system for sound velocity measurement (e.g.…”
Section: Transducer Modellingmentioning
confidence: 99%
See 1 more Smart Citation
“…Setting F i = −v i Z m,i , this enables to solve equation ( 4) for the frequency-dependent electrical impedance Z el = u/i of the transducer model. In an inverse procedure, the parameters of the Mason model for a given ultrasonic transducer are identified by comparing the electrical impedance of the model Z el with the electrical impedance Z meas of a physical transducer [4]. As the physical transducer is to be used in an acoustic absorption measurement system based on an established system for sound velocity measurement (e.g.…”
Section: Transducer Modellingmentioning
confidence: 99%
“…Note that these results are only valid for the setup and transducer described before with an excitation signal voltage of 1 V. As a reference, the specific acoustic impedances and losses of several fluids at 293 K and 100 kPa are included in figure 3 as well [7]. The losses µ depicted are low estimates, as they only include the influence of shear viscosity and thermal conductivity (µ = 4 3 µ s + cp−cv cp•cv ν), omitting the additional loss caused by the relatively unexplored volume viscosity. Thus, in a physical setup, the difference between the minimal losses necessary for linear sound propagation and the actual losses in the respective fluid is expected to be more significant.…”
Section: Estimation Of Non-linearitymentioning
confidence: 99%
“…For details regarding the inverse problem and optimization of sensitivities see e.g. [5], [7]. In order to design and analyse new piezoelectric devices, models are employed [14].…”
Section: Introductionmentioning
confidence: 99%