<oai_dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
  <dc:creator>Chilukoti, Hari Krishna</dc:creator>
  <dc:creator>Zhou, Tianhang</dc:creator>
  <dc:creator>Ardham, Vikram Reddy</dc:creator>
  <dc:creator>Böhm, Michael C.</dc:creator>
  <dc:creator>Müller-Plathe, Florian</dc:creator>
  <dc:date>2019-12-05</dc:date>
  <dc:description xmlns:ns0="xml" ns0:lang="en">Molecular dynamics simulations have been performed to investigate the mechanism  of thermal energy transport at the interface between n-heneicosane in solid and liquid  phases and few-layer graphene at different temperatures under two heating modes (in  the “heat-matrix” mode, heat is flowing from the heated heneicosane molecules to the  cooled ones through the graphene layers and in the “heat-graphene” mode, the  energy is flowing from the heated graphene to the cooled heneicosane). The effect of  orientation of the perfect crystal structure (heneicosane molecules are positioned  perpendicular and parallel to the graphene basal plane) on the interfacial thermal  conductance has been examined. It is observed that the interfacial thermal  conductance is 2 orders of magnitude higher under the heat-matrix mode than under  the heat-graphene mode, for liquid or solid heneicosane and monolayer graphene.  With an increase in the number of graphene layers, the interfacial thermal  conductance under the heat-matrix mode decreases and reaches a plateau when the  number of the graphene layer is more than eight. This is caused by the decreasing  contribution of direct heat transfer from the matrix to matrix across the graphene  layers via nonbonded intermolecular interactions. The interfacial thermal conductance  becomes similar for both heating modes, once the number of graphene layers in the  system is over 15. The influence of temperature on the interfacial thermal  conductance is found to be insignificant in the range (175–250 K; 350–400 K). Both  the phase and structure of heneicosane significantly influence the interfacial  conductance. Spectral analysis suggests that graphene vibrational modes of all  frequencies contribute to the interfacial heat transfer.</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>https://folia.unifr.ch/global/documents/308294</dc:identifier>
  <dc:identifier>https://folia.unifr.ch/documents/308294/files/ard_tet.pdf</dc:identifier>
  <dc:identifier>https://folia.unifr.ch/documents/308294/files/ard_tet_sm.pdf</dc:identifier>
  <dc:language>eng</dc:language>
  <dc:relation>info:eu-repo/semantics/altIdentifier/doi/10.1021/acs.jpcc.9b07054</dc:relation>
  <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
  <dc:rights>License undefined</dc:rights>
  <dc:source>The Journal of Physical Chemistry C. - 2019, vol. 123, no. 48, p. 29192–29202</dc:source>
  <dc:subject>info:eu-repo/classification/udc/54</dc:subject>
  <dc:title xmlns:ns1="xml" ns1:lang="en">Thermal energy transport across the interface between phase change material n-heneicosane in solid and liquid phases and few-layer graphene</dc:title>
  <dc:type>http://purl.org/coar/resource_type/c_6501</dc:type>
</oai_dc:dc>
