Polymer Nanocomposite Materials. Группа авторов

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alt="Cyclic vapor sensing behavior of the nanofiber composite with different SEBS contents to different vapors including: (a) THF, (b) toluene, and (c) heptane. Source: (a)–(c) Reproduced with permission. [116] Copyright 2018, The Royal Society of Chemistry. (d) Photos of a volunteer wearing the integrated mask, and the mask incorporated with CNC-based humidity sensor. (e) Vapor sensing behavior of the sensor to fast, normal, and deep breathing and (f) mouth and nose breathing. Source: (d)–(f) Reproduced with permission. [155] Copyright 2019, American Chemical Society."/>

      2.4.4 Temperature Sensor

      CPCs served as temperature sensors show many popular applications for thermal detectors, over-temperature protection devices and self-regulating heaters, etc. [158]. The temperature sensing behavior of CPCs is based on positive temperature coefficient (PTC) effect and negative temperature coefficient (NTC) effect. Conceptually, PTC and NTC of thermistors display a conspicuous increase and a succeeding gradual decrease in electrical resistance with increasing temperature, respectively [122]. It is believed that the PTC effect arises from the expansion or the melting of the matrix, which would increase the distance between conductive elements. While a flocculated structure formed at elevated temperatures, resulting in NTC effect.

(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.

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