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Online proceedings - EDA Publishing Association

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The XRD shows a peak above the 2θ = 20˚ angle associated<br />

with the α-phase, but well lower than the 2θ = 21˚ associated<br />

with the β-phase Clearly the PVDF hasn’t made the complete<br />

transition from alpha phase to beta phase, but it may have<br />

started the transition. In a number of samples we experienced<br />

PVDF precipitates or other imperfection, such as small voids<br />

which disqualified the samples from further testing. As for<br />

FTIR measurements no clear interpretation has been obtained<br />

between unpoled and poled PVDF for our test samples. The<br />

test sample of gold coated PVDF membrane has withstood<br />

over an hour of testing in the flexing test jig and shows no<br />

signs of fatigue yet. Ultimately, the details for applying PVDF<br />

to the fabric substrate require waiting until we identify the best<br />

method for poling the PVDF solvent while curing and in situ.<br />

One of last test suggests dominant d 33 [9] properties as it<br />

stretched in the test jig showing piezoelectricity, as opposed to<br />

the d 31 parameter that we are looking for. This is important<br />

due to the method of deformation. What is occurring is<br />

stretching as opposed to bending as would be natural with a<br />

fabric. The membrane is clearly piezoelectric, as can be seen<br />

in Fig. 8, but not yet in the β-phase required for better power<br />

generation.<br />

11-13 May 2011, Aix-en-Provence, France<br />

<br />

<br />

APPENDIX<br />

David Elam<br />

Greg Collins<br />

James Benson<br />

Dr. C.L. Chen<br />

Dr. A. Chabanov<br />

ACKNOWLEDGMENT<br />

4<br />

Fig. 8. Voltage generated from membrane at 1 Hz frequency.<br />

VII. CONCLUSION<br />

The membrane generated a charge due to its piezoelectricity.<br />

The in-situ poling and curing show promise largely because<br />

PVDF shrinks during curing, causing stress, strain. We<br />

continue to test new methods such as developing better in situ<br />

preparation of poling, curing, and heating simultaneously. We<br />

hope to complete the α-phase to β-phase process transition as<br />

efficiently as possible and apply that technique to the FlecTron<br />

fabric. Further research activities will consist of thin film<br />

optimization to maximize charge generation as well as<br />

extended testing to determine the useful life of the membranes<br />

produced. This is just the beginning of research into<br />

piezoelectric materials and applying what we learn towards<br />

improving our quality of life.<br />

REFERENCES<br />

[1] I. Elashmawi, N. Elsheshtawi, H. Abdelkader, N. Hakeem, Cryst. Res.<br />

Tech 2007, pp. 157–163<br />

[2] A. Kumar, and M. Perlman, J. Phys. D: Appl. Phys. 1992, pp.469-475<br />

[3] Y. Huan, Y. Liu, and Y. Yang, Polymer Eng. And Science 2007,<br />

pp.1630-1633<br />

[4] V.Sencadas, S. Lanceros-Mendez, J. Mano, Thermochimica Acta 2004,<br />

pp.201-207<br />

[5] V. Kochervinskii, V. Volkov, and K. Dembo, Physics of Solid State<br />

2006, pp. 1083-1085 (any par)<br />

[6] W. Yu, Z. Zhao, W. Zheng, B. Long, Q. Jiang, G. Li, X. Ji, Polymer<br />

Engineering and science 2009, pp.491-498<br />

[7] Y. Liu, G. Tian, Y. Wang, J. Lin, Q. Zhang, and H. Hoffmann, J.<br />

Intelligent Mat. Systems and Structures 2009, pp. 575-585<br />

[8] W. Ma, J. Zhang, X. Wang, and S. Wang, Applied Surface Science 2007,<br />

pp. 8377-8388<br />

[9] V. Kochervinskii, Crystallography Reports 2003, pp. 649- 675<br />

[10] Z. Wang, and J. Miao, J. Phys D: Appl. Phys. 2008, pp. 41-47<br />

141

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