By Edited by: Assoc. Costas Sikalidis

ISBN-10: 9533073500

ISBN-13: 9789533073507

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The driving chains (Figure 5) connect the free joints of the links n 0B of the basic parallel chain in between them. The number of the driving chains in this case is defined by the difference (9) as: m = i. The kinematic structures defined as a result of synthesis for n0=2, 3 and i =1, 2 according Table 1 are shown graphically in Table 4 on the left. On the right of Table 4 the possible kinematic structures are shown for case i =1, 2 and the number of the links of basic parallel chain n 0B = 3.

The polarised ceramic elements can be estimated as actuators for linear motion, which can be modelled by the kinematic chain shown in Figure 5. It includes two links 1 and 2 and a joint T with linear motion, which can perform drive functions and two rotational joints R by which the actuator is attached to the driven links. The rotational joints can be created by introducing elastic areas in the ceramics or by additional elastic joints. Advances in Ceramics – Electric and Magnetic Ceramics, Bioceramics, Ceramics and Environment 30 R 1 T 2 R Fig.

A rapid and low-field resonance method eliminates the displacement due to polarization rotation. The dynamic d33 values calculated from the linear part of the slope under a high field of more than 20 kV/cm are 200-350 pm/V generally. These values roughly correspond to twice the d31 value calculated by the resonance method, indicating that the explanations above are reasonable. Qm is related to the internal stress. 04 Electric field (kV/cm) Fig. 21. Polarizations and field-induced strains of the BT ceramics two-step-sintered at (a) 1300 and (b) 1400 °C.

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Advances in Ceramics - Electric and Magnetic Ceramics, Bioceramics, Ceramics and Environment by Edited by: Assoc. Costas Sikalidis


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