Download Advances in Woven Fabrics Technologies by S. Vassiliadis PDF

By S. Vassiliadis

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J. (2002). Semiconducting and metallic polymers: the fourth generation of polymeric materials. Synth. Met. No. 125, pp. 23-42. , Cheeseman, B. , Popper, P. -W. (2000). Some recent advances in the fabrication and design of three-dimensional textile preforms: a review. Composites Science and Technology, Vol. 60, pp. 33-47. Kirkpatrick, S. (1973). Percolation and conduction. Reviews of Modern Physics, Vol. 45, No. 4, pp. 574-588. Ko, F. (2007). 3-D textile reinforcements in composite materials, 3-D Textile Reinforcements In Composite Materials.

Conductive fibres and conventional (non-conductive) fibres are needed alongside piezoelectric fibres. Because piezoelectric fibres carry negative charges on one side along its length and positive charge on the other side, a conductive material is needed to carry the charge produced by Smart Woven Fabrics in Renewable Energy Generation 31 movements of the piezoelectric fibres. Conductive wires would add extra rigidity to the fabric which is an undesirable outcome for most textile structures. The best alternative to undesirable wires may be conductive fibres are produced and patented (Perera & Mauretti, 2009).

For all four fabric designs studied in this chapter, interlace of piezoelectric and conductive fibre/yarn is significant. In a woven fabric structure, one piezoelectric fibre can interlace with more than one conductive fibre and one conductive fibre can also interlace with more than one piezoelectric fibre. However, to avoid any short circuit, one conductive fibre can only interlace with the same pole of the each piezoelectric fibre. Since the fibres are considered having the same thickness, in the first design, piezoelectric and conductive fibres interlace 96 times in the fabric.

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