2018
DOI: 10.1088/1361-665x/aae8fb
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Properties of piezoceramic materials in high electric field actuator applications

Abstract: In this paper, we compare the performance of 8 PZT ceramics and one PMN-PT material for typical bending actuator applications. This includes the measurement of nonlinear transverse charge coefficient at high electric field strength and related quantities such as the Young's modulus, relative permittivity, coercive field and their temperature dependencies, and the Curie temperature. Most materials show much higher strains than what is expected from the datasheet values. We further study the operating region for… Show more

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Cited by 38 publications
(37 citation statements)
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“…The time-dependent study was selected in the simulation as the velocities, which are used in the moving mesh module, are time-dependent values, and as the stationary study does not compute these instantaneous velocities. In the study, the time range was selected from 0 s to 1 s with a step of 0.1 s. The applied voltages were limited to 140 V in positive polarization direction, and −40 V in negative polarization direction to avoid piezo saturation and re-polarization [19]. A sinusoidal voltage within the voltage limits was defined using a piecewise function under global definitions.…”
Section: Resultsmentioning
confidence: 99%
“…The time-dependent study was selected in the simulation as the velocities, which are used in the moving mesh module, are time-dependent values, and as the stationary study does not compute these instantaneous velocities. In the study, the time range was selected from 0 s to 1 s with a step of 0.1 s. The applied voltages were limited to 140 V in positive polarization direction, and −40 V in negative polarization direction to avoid piezo saturation and re-polarization [19]. A sinusoidal voltage within the voltage limits was defined using a piecewise function under global definitions.…”
Section: Resultsmentioning
confidence: 99%
“…Because of the non-linearity of the piezoelectric charge coefficient d 31 and the hysteresis and creep effects, we did not simply use a constant d 31 , but we needed to determine the charge coefficient as a function of the applied voltage and its voltage history. For this reason, we followed the established strategy of [32] and manufactured a simple mono-morph bending beam with one 100 µm thick passive glass layer and one Ekulit piezo layer that we could simulate reliably. We applied the same electric fields as for the lens measurements (see section 5) to this beam, measured the beam curvature and compared it to the simulation as done in [32].…”
Section: Piezoelectric Non-linearitymentioning
confidence: 99%
“…As a piezo material, we detach the piezo sheets from Ekulit sound buzzers with the mentioned small thickness of t = 105 µm to achieve high focal powers referring to equation (4). They in fact showed better performance with a high piezoelectric coefficient of d 31 ≈ −487 pm V [32] for high electric fields and a better surface quality than many readily available raw piezo foils. We used this value for all analytical calculations but need to be aware that for small electric fields, the piezoelectric coefficient is reduced by up to 40 % [32] resulting in overestimated focal powers in the bending mode.…”
Section: Fabricationmentioning
confidence: 99%
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