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Composite Materials Research Progress

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266 Yasuhide Shindo and Fumio Narita<br />

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Figure 6. Displacement versus voltage for laminated actuator.<br />

Next, the effect of electrode length on the performance of the actuator with L = 30 mm,<br />

W = 10 mm and 4h = 20 mm is discussed. Fig. 6 shows the predictions of displacement<br />

uz at x =0mm, y =0mm and z =10mm as a function of applied voltage V0, based on<br />

work, for a =20, 24 and 28 mm. Non-linearity in the displacement versus voltage curves<br />

depends on the electrode length. The displacement increases with an increase of a from 20<br />

mm to 24 mm. Little difference is observed between the results for a =24mm and 28 mm.<br />

4. Piezoelectric Disk <strong>Composite</strong>s<br />

4.1. Problem Statement and Solution Procedure<br />

Consider a two-layered piezoelectric disk composite with radius c and thickness h as shown<br />

in Fig. 7. The origin of the coordinates (r,θ,z) is located at the center of the interface<br />

considered as z =0, 0 ≤ r ≤ c. The z axis is assumed to coincide with the six fold<br />

axis of symmetry in the class of a 6mm crystal class, or with the poling axis in the case<br />

of poled piezoelectric ceramics. Three parallel circular electrodes of radius b lie in the<br />

planes z =0, ±h. The bonding at z =0is assumed to be perfect so that the stresses and<br />

displacements are continuous along the interface of the composite. Let the voltage applied<br />

to the internal electrode surface be denoted by V0. The surface electrodes are grounded.<br />

The axisymmetric models were generated using the commercial FE method software<br />

package. The electrode layers were not incorporated into the model.

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