Piezoelectric Ceramic Essay

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In a piezoelectric cantilever, the poled directions of the piezoelectric layers are usually perpendicular to the planar direction of the piezoelectric layers because it is the most convenient way to polarize piezoelectric sheets when they are fabricated. Piezoelectric cantilevers operating in the above manner are said to be operating in the “31 mode,” where “3” denotes the polarization direction of the piezoelectric layer and “1” denotes the direction of the stress, which is primarily material, d31 is always smaller than d33 because in the 31 mode the stress is not applied along the polar axis of the piezoelectric material [3]. Therefore, in order to utilize a piezoelectric sheet in the “d33” mode for higher energy output, an interdigitated …show more content…

Application of an electric field across the ceramic creates a mechanical strain, and in a similar manner, application of a mechanical stress on the ceramic induces an electrical charge [4]. The fundamental component of a piezoelectric stack actuator is a wafer of piezoelectric material sandwiched between two electrodes. Prior to fabrication, the wafer is polarized uniaxially along its thickness, and thus exhibits significant piezoelectric effect in this direction only. A typical piezoelectric stack actuator is formed by assembling several of the wafer elements in series mechanically and connecting the electrodes so that the wafers are in parallel electrically, as illustrated in figure 5 [4]. The nominal quasi-static behaviour of a piezoelectric stack actuator is a steady-state output displacement that is monotonically related to the voltage …show more content…

Thus, a structronic shell is an active and adaptive system whose static and dynamic characteristics can be actively tuned and controlled to meet its performance requirement as uncertain circumstances occur [5]. Piezoelectric shells, continua, and distributed systems have been investigated for years and their theories and mathematical models are relatively well established. Electrostrictive effects in ferroelectric material were first observed in early 50s. Electrostrictive shells were initially evaluated and mathematical models were established. Unlike the linear dependence of piezoelectric materials, the induced strain in electrostrictive material is a quadratic function of applied electric field [5]. The low hysteresis and the high induced actuation authority of electrostrictive actuators would potentially contribute a breakthrough in actuation and control applications. However, there are certain ferroelectric materials, e.g., barium titanate (BaTiO3), possessing dual electrostrictive and piezoelectric characteristics depending on the Curie

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