fig6

Unlocking the potential of liquid crystals as phase change materials for thermal energy storage

Figure 6. Dependence of phases of liquid crystals and additives (e.g., nanomaterials) in liquid crystals on the thermal conductivity. Thermal conductivity as a function of temperature for homeotropic (k, red dots) and planar (k||, black dots) configurations of the (A) 5CB (the vertical line is the nematic-to-isotropic transition line, TNI = 35.17 °C), and (B) 9CB molecules. (A) Reproduced with permission from ref.[130]. Copyright (1994) by the American Chemical Society. (B) Reproduced with permission from ref.[131]. Copyright (1998) by the American Chemical Society. (C) Thermal conductivity of dimeric coumarin liquid crystals. (D) Thermal conductivity of dimeric coumarin liquid crystal (carbon no. in R = 14) mixed with alumina (Al2O3) nanoparticles and boron nitride (BN) nanosheets. Reprinted from ref.[132], Copyright (2023), with permission from Elsevier.

Energy Materials
ISSN 2770-5900 (Online)
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