Thermally conductive phase change nanocomposites presenting PS-PEG/ SeO2 and PS-PEG/BN/SeO2

buir.contributor.authorMutlu, Saliha
buir.contributor.authorOrtaç, Bülend
buir.contributor.authorYılmaz, Sevil Savaşkan
buir.contributor.orcidMutlu, Saliha|0000-0002-5097-5450
buir.contributor.orcidOrtaç, Bülend|0000-0002-1104-7459
buir.contributor.orcidYılmaz, Sevil Savaşkan|0000-0002-1055-7799
dc.citation.epage176291-19
dc.citation.spage176291-1
dc.citation.volumeNumber1007
dc.contributor.authorMutlu, Saliha
dc.contributor.authorOrtaç, Bülend
dc.contributor.authorBaşkan, Taylan
dc.contributor.authorYılmaz, Sevil Savaşkan
dc.contributor.authorYılmaz, Ahmet Hakan
dc.date.accessioned2025-02-21T11:48:39Z
dc.date.available2025-02-21T11:48:39Z
dc.date.issued2024-12-05
dc.departmentInstitute of Materials Science and Nanotechnology (UNAM)
dc.description.abstractThe phase change and thermal conductivity properties of nanocomposite materials consisting of cross-linked Poly(Styrene-block-Ethylene Glycol Dimethyl Methacrylate) (PS-PEG DM), boron nitride (BN), and selenium dioxide (SeO$_2$) were investigated in this study. The different content of phase-changed materials (PCM) nanocomposites was prepared by using the hydraulic pressure technique. Promising melting enthalpy values (104.5, 98.8 and 165.8 J g$^{-1}$) have been reached for P1Se3, P2BN2Se2, and P3BN2Se2 PCM nanocomposites. The enthalpy efficiencies associated with the processes of melting and freezing, denoted as λ$_m$ and λ$_c$, respectively, were determined by the analysis of data obtained from DSC. Our study was demonstrated to present comprehensive information on the PS-PEG/BN, PS-PEG/SeO2, and PS-PEG/BN/SeO2 phase change nanomaterials, thereby facilitating their potential applications in various fields. The phase change and thermal conductivity properties of PS-PEG/BN/SeO$_2$ nanocomposites were investigated. The incorporation of SeO2 and BN nanoparticles significantly enhanced the thermal conductivity (for P2BN4Se5), reaching values up to 8.277 W m$^{-1}$ K$^{-1}$. The λ$_m$ values of P1Se3, P2BN2Se2, and P3BN2Se2 were calculated as 68.79, 61.23, and 87.86, respectively. The λ$_c$ values of P2Se3; P1BN2Se2 were also calculated at 70.10; 98.93 and 161.92, respectively.
dc.embargo.release2026-12-05
dc.identifier.doi10.1016/j.jallcom.2024.176291
dc.identifier.eissn1873-4669
dc.identifier.issn0925-8388
dc.identifier.urihttps://hdl.handle.net/11693/116566
dc.language.isoEnglish
dc.publisherElsevier BV
dc.relation.isversionofhttps://doi.org/10.1016/j.jallcom.2024.176291
dc.rightsCC BY 4.0 DEED (Attribution 4.0 International)
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/
dc.source.titleJournal of Alloys and Compounds
dc.subjectThermal conductivity
dc.subjectPhase change materials
dc.subjectPolymer-boron nitride-selenium dioxide nano-composite
dc.subjectPolystyrene-polyethyleneglycol block
dc.subjectCopolymer
dc.subjectEnthalpy efficiency
dc.subjectHeat capacity
dc.titleThermally conductive phase change nanocomposites presenting PS-PEG/ SeO2 and PS-PEG/BN/SeO2
dc.typeArticle

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