Polymer Nanocomposite Materials. Группа авторов

Polymer Nanocomposite Materials - Группа авторов


Скачать книгу
of CPPC/CB foam and the NTC effect declines with the increase of CB content. The schematic diagram of temperature sensing mechanism for the CPPC/CB foam composite is demonstrated in Figure 2.10c. The cell walls of the foam were squeezed by expanded gas and the thickness of the cell walls was reduced during the heating. Therefore, the distance between adjacent CB particles was decreased and more conductive pathways formed in polymer matrices, leading to the decrease of the resistance.

(a) The normalized resistance (R/R0) variation with temperature from 25 to 70 °C for the solid CB/CPPC composites with 2.5 vol% CB. (b) The normalized resistance (R/R0) variation with temperature from 25 to 70 °C for CPPC/CB foams with 0.20, 0.30, and 0.45 vol% CB. (c) Schematic illustration of microstructural evolution in CPPC/CB foams during heating process. Source: (a)–(c) Reproduced with permission. [159] Copyright 2018, The Royal Society of Chemistry. (d) The curve of resistivity vs. temperature for the HDPE/CB (80/20) with different content of GNFs. (e) The curve of resistivity vs. temperature for the HDPE/CB (75/25) with different content of GNFs. Source: (d)–(e) Reproduced with permission. [160] Copyright 2009, Elsevier Ltd.

      The temperature-resistivity intensity (intensity of positive temperature coefficient [IPTC] and intensity of negative temperature coefficient [INTC]) of CPCs is an essential index for temperature sensors. A low INTC value is required for a preferable temperature sensor to output large response toward temperature stimuli [161]. To increase the IPTC intensity, many efforts have been made to remove the NTC effect. It is accepted that the NTC effect is due to the reaggregation of the conductive nanofillers in the polymer matrix and recovery of disconnected conductive pathways [162]. The usual method is using crosslinking agent or radiations, which could increase the viscosity of polymer matrix and prevent the reaggregation of conductive fillers, thus eliminating the NTC effect [163, 164]. Lu et al. [162] fabricated nylon6 (PA6)/PS/(poly(styrene-co-maleic anhydride) (SMA)–CB) composite with especial interface morphology. The PA6/PS/(SMA–CB) composites showed stronger IPTC than PA6/PS/CB and NTC effect was eliminated. The special interfacial morphologies and low percolation threshold are responsible for elimination of NTC and stronger IPTC.

      Due to its inherent properties of lightweight, low cost, easy fabrication, and controllable resistance, CPCs have been the research hotspot in the past decades. The incorporation of different conductive nanofillers like CNTs, graphene, silver nanoparticles, and silver nanowires greatly enhances the electrical property of CPCs. However, fabricating high performance CPCs still remains a great challenge, because conductive fillers, especially nano-sized conductive particles, are easy to aggregate in the polymer due to their high-aspect ratio, resulting in uneven distribution of fillers.

      Nanofiller aggregations would affect or even worsen the performance of CPC. Thus, even dispersion of conductive nanofillers in the polymer matrix is a vital issue. Here, surface modification of nanofillers and special processing technique are raised: (i) the physical blending, (ii) in situ polymerization, (iii) chemical modification of conductive filler, and (iv) introduced surfactant. All of the aforementioned methods can improve the dispersion of conductive particles in polymer, but there are still many disadvantages. Method (i) the polymer may be partially degraded under high shear strength. In addition, when the external force stops, the conductive particles will reunite. In method (ii), the solvent should be carefully chosen, that is, the selected solvent can not only dissolve the polymer monomer and its initiator, but also disperse the conductive filler well. In method (iii), the chemical modification of conductive particles is complicated and the yield is low. The introduction of surfactants in method (iv) may have adverse effects on the mechanical and other properties of polymer materials. Therefore, improving the dispersion of conductive particles in polymer is still a key problem in CPC preparation.

      The flexibility, light weight, and controllable network structure endow the CPCs with potential applications in sensing including strain sensors, piezoresistive sensors, gas sensors, and temperature sensors. With the development of artificial intelligence (e.g. electronic skin and human–machine interface), skin adhesive and mechanically flexible CPCs with multi-functionality will become a new hotspot.

      1 1 Zhang, Y., Pan, T., and Yang, Z. (2020). Flexible polyethylene terephthalate/polyaniline composite paper with bending durability and effective electromagnetic shielding performance. Chem. Eng. J. 389: 124433.

      2 2 Lim, Y.W., Jin, J., and Bae, B.S. (2020). Optically transparent multiscale composite films for flexible and wearable electronics. Adv. Mater. 32: 1907143.

      3 3 Chen, J., Yu, Q., Cui, X. et al. (2019). An overview of stretchable strain sensors from conductive polymer nanocomposites. J. Mater. Chem. C 7: 11710–11730.

      4 4 Shirakawa, H. (2001). The discovery of polyacetylene film: the dawning of an era of conducting polymers (Nobel lecture). Angew. Chem. Int. Ed. 40: 2574–2580.

      5 5 Tang, C., Chen, N., and Hu, X. (2017). Conducting polymer nanocomposites: recent developments and future prospects. In: Conducting Polymer Hybrids, 1–44. Springer International Publishing.

      6 6 Erdem, E., Karakışla, M., and Sacak, M. (2004). The chemical synthesis of conductive polyaniline doped with dicarboxylic acids. Eur. Polym. J. 40: 785–791.

      7 7 Han, M.G. and Im, S.S. (2001). Dielectric spectroscopy of conductive polyaniline salt films. J. Appl. Polym. Sci. 82: 2760–2769.

      8 8 Kim, B.R., Lee, H.-K., Park, S., and Kim, H.-K. (2011). Electromagnetic interference shielding characteristics and shielding effectiveness of polyaniline-coated films. Thin Solid Films 519: 3492–3496.

      9 9 An,


Скачать книгу