Modified ballistic–diffusive equations for obtaining phonon mean free path spectrum from ballistic thermal resistance: I. Introduction and validation of the equations

Oh Myoung Kwon, Geoff Wehmeyer, Chris Dames

Research output: Contribution to journalArticle

Abstract

Phonon mean free path (MFP) spectra are essential for the accurate prediction and utilization of the classical size effect. Rebuilding an MFP spectrum from experimental data remains challenging. It requires solving the thermal transport phenomenon of a heat source of a given shape across the entire size range. Herein, to do this for a heat source embedded in an infinite medium, we derive a new set of modified ballistic–diffusive equations by analyzing the cause of the erroneous results observed in a steady-state solution of the original ballistic-diffusive equations. We demonstrate their ease and accuracy by obtaining the effective thermal conductivity for a spherical nanoparticle embedded in an infinite medium in an explicit closed-form and comparing it with that obtained by the Boltzmann transport equation (differences estimated as <3%).

Original languageEnglish
JournalNanoscale and Microscale Thermophysical Engineering
DOIs
Publication statusPublished - 2019 Jan 1

Fingerprint

thermal resistance
heat sources
Ballistics
Heat resistance
mean free path
ballistics
Boltzmann transport equation
thermal conductivity
Difference equations
nanoparticles
causes
Thermal conductivity
predictions
Nanoparticles
Hot Temperature

Keywords

  • ballistic thermal resistance
  • ballistic–diffusive equations
  • effective thermal conductivity
  • Phonon mean free path
  • phonon mean free path spectrum

ASJC Scopus subject areas

  • Atomic and Molecular Physics, and Optics
  • Materials Science(all)
  • Condensed Matter Physics
  • Mechanics of Materials

Cite this

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AB - Phonon mean free path (MFP) spectra are essential for the accurate prediction and utilization of the classical size effect. Rebuilding an MFP spectrum from experimental data remains challenging. It requires solving the thermal transport phenomenon of a heat source of a given shape across the entire size range. Herein, to do this for a heat source embedded in an infinite medium, we derive a new set of modified ballistic–diffusive equations by analyzing the cause of the erroneous results observed in a steady-state solution of the original ballistic-diffusive equations. We demonstrate their ease and accuracy by obtaining the effective thermal conductivity for a spherical nanoparticle embedded in an infinite medium in an explicit closed-form and comparing it with that obtained by the Boltzmann transport equation (differences estimated as <3%).

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