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Thermal transport and crystallisation in octadecane composites with porous framework coatings and graphene

Hind AlbalawiDepartment of Physics, College of Sciences, Princess Nourah bint Abdulrahman University, P.O. Box 84428, 11671, Riyadh, Saudi ArabiaAzfarizal MukhtarInstitute of Sustainable Energy, Putrajaya Campus, Universiti Tenaga Nasional, Jalan IKRAM-UNITEN, 43000, Kajang, MalaysiaSanatjon JafarovUrgench State University, Kh. Alimdjan Str. 14, 220100, Urgench, UzbekistanDilshodbek SotvoldiavUniversity of Tashkent for Applied Sciences, Str. Gavhar 1, 100149, Tashkent, UzbekistanAsilbek AbdullayevKimyo International University in Tashkent, Shota Rustaveli Str. 156, 100121, Tashkent, UzbekistanAlisher AbduvokhidovAndijan State University, Universitet Str. 129, 170100, Andijan, UzbekistanBharosh Kumar YadavDepartment of Mechanical Engineering, Purwanchal Campus, Institute of Engineering (IOE), Tribhuvan University (TU), Dharan-08, Kiritipur, Nepal
2026en
ABI

Annotatsiya

Low thermal conductivity and leakage limit the use of organic phase change materials for latent heat storage. Confinement can also delay crystallisation. Polyurea capsules containing n-octadecane were coated with either zeolitic imidazolate framework-8 (ZIF-8) or Universitetet i Oslo-66 (UiO-66) and embedded in a polyurethane matrix containing graphene nanoplatelets. Modulated differential scanning calorimetry characterised heat-flow components, while fast scanning calorimetry examined cooling-rate dependence. At a graphene loading of 5 wt%, the ZIF-8-coated composite had an effective thermal conductivity of 0.78 ± 0.04 W m −1 K −1 at 25 °C and an onset-based supercooling of 1.2 ± 0.2 °C. Corresponding values for the UiO-66-coated composite were 0.72 ± 0.03 W m −1 K −1 and 2.4 ± 0.3 °C. Control composites containing only the coating or only the graphene reached 0.31 ± 0.02 and 0.44 ± 0.03 W m −1 K −1 , so neither component accounts for the transport of the complete formulation. The ZIF-8-coated composite retained 98.2 ± 1.1% of its initial melting enthalpy after 1000 cycles between 10 and 60 °C, losing 0.34 ± 0.08% of its mass and showing unchanged infrared and diffraction signatures. Values are means and standard deviations across three independently prepared batches. The two coatings differ in thickness, crystallite size, surface area and growth conditions, so the measurements compare complete formulations rather than isolating a topology-dependent nucleation mechanism. Discharge power at device scale remains untested.

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