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Articles

Modified Ballistic–Diffusive Equations for Obtaining Phonon Mean Free Path Spectrum from Ballistic Thermal Resistance: II. Derivation of Integral Equation Based on Ballistic Thermal Resistance

, &
Pages 334-347 | Received 06 Dec 2018, Accepted 28 May 2019, Published online: 13 Jun 2019
 

ABSTRACT

Rebuilding phonon mean free path (MFP) spectra from experimental data is integral to phonon MFP spectroscopy. However, being based on effective thermal conductivity, the current integral equation for this precludes the use of certain heat sources of convenient shapes, such as a cylindrical nanoline. Herein, to enable using diverse specimens exhibiting a ballistic effect, we develop a ballistic thermal resistance-based integral equation, utilizing the ease and accuracy of the modified ballistic–diffusive equations demonstrated in the companion paper. The availability of more diverse shapes of specimens will enhance further development and widen use of phonon MFP spectroscopy.

Nomenclature

A=

area (m2)

C=

volumetric specific heat (J/m3∙K)

D=

characteristic length of a heater, density of states

f=

distribution function

ħ=

reduced Planck constant

j=

polarization index

k=

thermal conductivity (W/m∙K)

n=

the unit vector normal to the boundary

q=

heat flux (W/m2)

q˜=

nondimensional heat flux

q=

heat flux vector (W/m2)

r=

coordinate in r direction

r˜=

nondimensional coordinate in r direction

r=

position vector

s=

distance along the propagation direction

s˜ =

nondimensional distance along the propagation direction

S=

suppression function

t=

time

T=

temperature (K)

u=

specific internal energy (J/m3)

v=

group velocity (m/s)

v=

group velocity vector (m/s)

x=

coordinate in x direction

z=

coordinate in z direction

z˜=

nondimensional coordinate in z direction

Greek symbols

χχ=

a parameter defined as Λ/D

ϕ=

mean free path spectrum of a bulk medium or polar angle

ϕ˜=

normalized phonon mean free path spectrum

Λ=

mean free path

μ=

cosine of an angle θ

θ=

angle

τ=

relaxation time

τ1=

size parameter

ω=

angular frequency

Ω=

solid angle

Ωˆ=

direction vector

Subscripts

b=

ballistic

e=

emitting

eff=

effective value

F=

Fourier’s law

i=

incident

m=

diffusive

max=

maximum value

n=

normal

R=

based on ballistic thermal resistance

w=

wall or boundary

ω=

spectral property in terms of angular frequency

Additional information

Funding

This research was supported by the Nano-material Technology Development Program (No.2011-0030146) and Basic Science Research Program (NRF-2018R1A2B2002837) through the National Research Foundation of Korea (NRF) funded by the Ministry of Education, Science and Technology.

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