Polymer Composites for Electrical Engineering. Группа авторов
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СКАЧАТЬ serving as photon harvesters and molecular heaters have been proved to be good candidates for the fabrication of photodriven polymeric phase change composites. The working mechanism and experimental setup of solar‐to‐heat conversion associated with polymeric phase change composites are shown in Figure 2.7b. During the solar radiation from simulated light source, phase change composites can absorb thermal energy in the form of sensible heat, leading to a rapid increase in temperature. When the temperature reaches the phase change temperature, an inflection point emerges in the temperature evolution curves, indicating that phase transition and TES in the form of latent heat take place with small temperature fluctuation. After the phase transformation, the temperature rises again, and the converted heat energy is expressed as sensible heat in this phase. Upon removing the incident light, the temperature drops sharply and another phase change platform emerges later, demonstrating that the stored heat energy is released to maintain the temperature during the solidification. After that the temperature of the system slowly decreases to room temperature.

      Aside from photodriven polymeric solid–liquid phase change composites, Zhou et al.[75] developed a photothermal energy conversion system by introducing graphene into crosslinked PU solid–solid PCMs. When the content of graphene in the phase change composites increased from 0.5 to 9.1 wt%, the photothermal energy conversion efficiency of the system increased from 42.9 to 78.7% accordingly. Furthermore, multifunctional PU‐based phase change composites with zinc oxide (ZnO) and graphene aerogel were fabricated.[116] Owing to the enhanced photoabsorption from ZnO and graphene aerogel and electrical conductivity from graphene aerogel, the photo‐/electro‐thermal energy conversion efficiencies of the system containing the resultant polymeric solid–solid phase change composites were up to 80.1 and 84.4%, respectively.

      2.4.3 Magnetism‐to‐Heat Conversion

      where P is alternating magnetic field power.

      2.4.4 Heat‐to‐Electricity Conversion

      The above three systems are capable of converting other forms of energy into heat energy for storage. How to use the thermal energy collected and stored by PCMs? In 2015, Jiang et al.[108] creatively proposed a proof‐of‐concept thermoelectric conversion by combining phase change energy storage materials with n/p‐type semiconductors, achieving the conversion of heat into applicable electricity. As shown in Figure 2.7d, the thermal energy from heat source can be collected and stored by PCMs, and then the collected heat is transferred to a commercial thermoelectric device, forming a temperature difference at its two ends and generating electricity via Seebeck effect. Similarly, Yu et al.[124] designed a thermoelectric energy conversion system based on graphene aerogel embedded shape‐stabilized PCMs. Two PCMs (PEG and 1‐tetradecanol) with different phase transition temperatures are, respectively, used as heat and cold sources at the ends of thermoelectric devices to tune the temperature difference. Based on the experimental data and numerical predictions, the heating and cooling energy conversion efficiencies are 52.81 and 30.29%, respectively. Furthermore, one‐step photo‐to‐electricity conversion systems (Figure 2.7e)[66, 104, 105] integrating light‐to‐heat with heat‐to‐electricity have been developed. To achieve light‐to‐heat‐to‐electricity energy conversion, a prerequisite is that phase change composites ought to possess excellent photoabsorption.

      Compared with electro/photo‐to‐heat energy conversion efficiency, magnetism‐to‐heat and heat‐to‐electricity conversion efficiencies are relatively low and need to be further improved. As the most of the above‐mentioned energy conversion systems are exposed to the surrounding environment, a portion of the converted heat energy is more or less dissipated, affecting the energy conversion efficiency. One solution is to carry out these energy conversion operations in a vacuum (thermal insulation) environment. Additionally, there is a lack of evaluation index for light‐to‐electricity energy conversion. For the case of photodriven phase change composites, polymer‐based photothermal absorbers such as artificial melanin, polyaniline (PANI), and polypyrrole (PPy) are competitive candidates. In heat/solar‐to‐electricity route, a commercial thermoelectric module is used directly, and thus an integrated device consisting of PCMs‐based component and thermoelectric component needs to be developed. Additionally, new ways of energy conversion associated with PCMs are waiting to be discovered.

      The foregoing energy conversion routes of PCMs are closely related to their practical applications. Polymeric phase change composites exhibit great potentials in thermal management of electronics,[61] smart textiles,[125] and shape memory devices[126].

Schematic illustration of potential applications of polymeric phase change composites. (a) Leakage-proof phase change composites as a temperature control component to prevent the chip from overheating and maintain a low working temperature.

      Source: Yang et al. [61]. Reproduced with permission from the American Chemical Society.

      (b) Flexible polymeric phase change composite fibers for personal thermoregulation textiles.

      Source: Wu et al. [127]. Reproduced with permission from the American Chemical Society.

      (c) PCMs‐based shape memory composites as a light‐actuated deployable roof for energy‐saving buildings.

      Source: Wu et al. [126]. Reproduced with permission from Elsevier Ltd.

      2.5.1 Thermal Management of Electronics