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Composite Materials Research Progress

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MV/m.<br />

Eletromechanical Field Concentrations and Polarization Switching... 269<br />

" # $ %" #<br />

Figure 11. Displacement versus voltage for disk composite tension actuator.<br />

the circular electrode tip, the normal stress at the interface is singular, and the stress ahead of<br />

the circular electrode tip is tensile, while the stress behind the electrode tip is compressive.<br />

The normal stress, apart from the interface, near the electrode tip has smaller value than the<br />

interface stress. Fig. 10 gives the distribution of the shear stress σzr as a function of r at<br />

z =0.01 and 0.2 mm for the same disk tension actuator. The magnitudes of the shear stress<br />

increase toward the circular electrode tip as is expected. Fig. 11 shows the predictions of<br />

displacement uz at r =0mm and z =1mm as a function of applied voltage V0, based<br />

on work, for b =8and 10 mm. There is a small influence of the electrode radius on the<br />

displacement versus voltage curves.<br />

Fig. 12 shows the computed strain εrr of C-91 + /C-91 + disk bending actuator corresponding<br />

to Fig. 8. The negative electric field increases the compressive strain, similar to<br />

C-91 + /C-91 − disk tension actuator. After the electric field reaches about −0.25 MV/m,<br />

polarization switching leads to a decrease in the compressive strain. As the electric field<br />

E0 continues to be reduced, the strain becomes tensile. On the other hand, as the positive<br />

electric field is increased, the strain near the electrode tip increases gradually due to the<br />

piezoelectric effect and then sharply increases as switching occurs due to electromechanical<br />

field concentrations. Little difference is observed between two criteria. Fig. 13 shows<br />

the predicted switching zones, based on work, near the circular electrode tip. As the electric<br />

fields increase, the area of the switched region grows. Fig. 14 shows the normal stress<br />

distribution σzz as a function of r at z =0and 0.2 mm for C-91 + /C-91 + disk bending<br />

actuator with b =8mm. The interface normal stress of the disk bending actuator is singular<br />

at the circular electrode tip, similar to the disk tension actuator. The stress ahead of<br />

the circular electrode tip is tensile, while the stress behind the circular electrode tip changes<br />

from tensile to compressive in the neighborhood of the electrode tip.<br />

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