By S. Vassiliadis
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Extra resources for Advances in Woven Fabrics Technologies
Piezoelectric Ceramics, Academic Press, London. R. H. (2010). Proceedings of SPIE – The International Society for Optical Engineering 7647. L. & Ounaies, Z. (2001). NASA ICASE Report No. 2001-28. Kawai, H. (1969). The piezoelectricity of poly(vinylidene fluoride), Jpn. 8, pp. ; Moll, F. (2005). J. Intell. Mater Syst. 16, pp. 835-845. Mauretti, G. J. & Perera, W. R. (2010). iCon Conductive Filaments, Proceeding of Textile Institute Centenary Conference, Manchester, UK, November 3-4, 2010 Neagu, E.
2007). Design and development of a flexible strain sensor for textile structures based on a conductive polymer composite. Sensors, Vol. 7, pp. 473-492. , & Koncar, V. (2010). A Flexible Strain Sensor Based on a Conductive Polymer Composite for in situ Measurement of Parachute Canopy Deformation. Sensors, Vol. 10, pp. 8291-8303. , Nagarajaiah, S. V. (2004). Nanotube film based on singlewall carbon nanotubes for strain sensing, Nanotechnology, vol. 15, pp. 379-382. , & Salagnac, P. (2005). Simulation of electrical and thermal behavior of conductive polymer composites heating elements.
Time. Fig. -% of CB from t = 0 s (Fig. 16-a) to t = 180 s (Fig. 16-f). Feeding voltage was constant and was equal to 15 V. Fig. 16 shows that comb structure (stainless steel yarn) heats first after switching on. The maximum temperature of this yarn was about 70 °C. This temperature is achieved after 120 s. CB coating heats relatively slowly but it can be conjectured that after 120 s the temperature of all the surface area exceeds 35 °C while it exceeds 40 °C after 180s. This behaviour is expected since stainless steel yarns have better thermal conductivity than carbon based composite.