Abstract

Piezopolymers with high piezoelectric responses are highly desirable for a broad range of sensor, actuator and transducer applications. Defects modification concept applied on PVDF yields a high transverse piezoelectric response with both high piezoelectric d <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">31</sub> (d <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">31</sub> =43.1pm/V) and electromechanical coupling k <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">31</sub> coefficients (k <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">31</sub> =0.187) in poly(\inylidene fluoride- hexafluoropropylene) [P(VDF-HFP)] 10wt% copolymers under quasi-static condition, much higher than these in the piezoelectric poly(vinylidene fluoride) (PVDF) and poly(\inylidene fluoride-trifluoroethylene) [P(VDF-TrFE)] copolymers. High frequency electromechanical resonance measurement was carried out under both LE mode and TE mode. Frequency dispersion of the piezoelectric response results in a smaller d31 (=20.5pm/V) at 50kHz. Thickness resonance measurement gives k <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">t</sub> =0.14 at 60MHz, which demonstrates it can be used as high frequency (>50MHz) ultrasonic transducers. Furthermore, the copolymers also display a higher d <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">31</sub> coefficient compared to the d <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">33</sub> coefficient, which seems to be unusual compared with most other piezopolymers. The experimental data suggests that the origin of the unusual piezoelectric response in these P(VDF-HFP) copolymers originates from a reversible change between a poled alpha-like structure and beta-like structure.

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