2019
DOI: 10.1016/j.ijheatmasstransfer.2018.11.064
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Interface thermal behavior in nanomaterials by thermal grating relaxation

Abstract: We study the relaxation of a thermal grating in multilayer materials with interface thermal resistances. The analytical development allows for the numerical determination of this thermal property in Approach to Equilibrium Molecular Dynamics and suggests an experimental setup for its measurement.Possible non-diffusive effects at the nanoscale are take into consideration by a non-local formulation of the heat equation. As a case study, we numerically apply the present approach to silicon grain boundary thermal … Show more

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Cited by 12 publications
(14 citation statements)
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References 39 publications
(68 reference statements)
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“…One can instead take advantage of the collected data for B2 and B3 in order to extrapolate our results using the equation developed by Alvarez and Jou [37]. This relationship describes the ballistic to diffusive regime inherent in non-local effects observed at small sizes in AEMD [38]:…”
Section: B Thermal Conductivity Via Aemd: Basic Foundations and Resultsmentioning
confidence: 99%
“…One can instead take advantage of the collected data for B2 and B3 in order to extrapolate our results using the equation developed by Alvarez and Jou [37]. This relationship describes the ballistic to diffusive regime inherent in non-local effects observed at small sizes in AEMD [38]:…”
Section: B Thermal Conductivity Via Aemd: Basic Foundations and Resultsmentioning
confidence: 99%
“…This behavior has been observed by AEMD in several other materials and nanostructures, and is related to nanoscale and non-local effects. 32 This can be rationalized in terms of behavior of heat carriers. Heat carriers with mean free paths (MFP) smaller than L are those experiencing scattering events, while transport is ballistic for heat carriers with a higher MFP.…”
Section: Thermal Transportmentioning
confidence: 99%
“…However, a compromise has to be found between a reliable treatment of the interatomic forces (requiring a first-principle description) and the computational ressources needed to follow in time the heat flux. To take advantage of the predictive power of FPMD and obtain the thermal conductivity at an accessible cost we employ AEMD in conjunction with FPMD [7][8][9] , as we have done successfully for amorphous GeTe 4 [10][11][12] and amorphous Ge 2 Sb 2 Te 5 13 . With this choice, the computational effort is reduced since the transient times inherent in AEMD are much shorter than the time intervals needed to treat the heat flux in alternative MD methods 14,15 .…”
Section: Introductionmentioning
confidence: 99%