Analytical expression for effective thermal conductivity of superlattices
Analytical expression for effective thermal conductivity of superlattices
Analytical expression for effective thermal conductivity of superlattices
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<strong>Analytical</strong> <strong>expression</strong> <strong>for</strong><br />
<strong>effective</strong> <strong>thermal</strong><br />
<strong>conductivity</strong> <strong>of</strong> <strong>superlattices</strong><br />
F. X. Alvarez, A. Lopeandia, J. Rodriguez-Viejo, D. Jou
Outline<br />
• Motivation<br />
• Introduction<br />
• Boundary resistance<br />
• Bulk <strong>conductivity</strong> modification<br />
• Results
Motivation<br />
Obtain an analytical and simple<br />
<strong>expression</strong> to predict <strong>thermal</strong><br />
<strong>conductivity</strong> <strong>for</strong> superlattice
Phonon<br />
• Mean free path<br />
• Coherence length<br />
• Wavelength<br />
l c<br />
l s<br />
l w
Phonon<br />
Boltzmann equation<br />
1/kBT<br />
Wave equation<br />
Wave equation
Large Phonons (Continuum/wave approx)
Small Phonons (Boltzmann eq approx)
Intermediate size Phonons (?)
Different behaviours<br />
• Ballistic - Diffusive<br />
• Coherent – Incoherent<br />
• Equilibrium – Non-equilibrium
Thermal <strong>conductivity</strong> <strong>of</strong> SL
Transmissivity<br />
( ) 2<br />
cos<br />
cos<br />
cos<br />
cos<br />
4<br />
j<br />
j<br />
j<br />
i<br />
i<br />
i<br />
j<br />
j<br />
j<br />
i<br />
i<br />
i<br />
S<br />
v<br />
v<br />
v<br />
v<br />
θ<br />
ρ<br />
θ<br />
ρ<br />
θ<br />
ρ<br />
θ<br />
ρ<br />
τ<br />
+<br />
=<br />
Specular<br />
Diffuse<br />
j<br />
j<br />
i<br />
i<br />
i<br />
i<br />
D<br />
v<br />
C<br />
C v<br />
C v<br />
+<br />
=<br />
τ
Transmission Coefficient<br />
Γ<br />
ijS<br />
/ D<br />
= ∫τ ( μ )<br />
ijS / D i<br />
μ<br />
i<br />
dμ<br />
i<br />
Γ = pΓ<br />
+ (1 − p)<br />
Γ<br />
ij<br />
ijS<br />
ijD
Mean Transmission Coefficient<br />
Γ =<br />
Γ + Γ<br />
12 21<br />
2<br />
Γ 12<br />
Γ 21
Transmission Coefficient
TBR<br />
R'<br />
=<br />
4<br />
π<br />
k<br />
4<br />
B<br />
2<br />
h<br />
ΓT<br />
3<br />
v<br />
2<br />
i<br />
3<br />
i<br />
∫<br />
0<br />
x Di<br />
x<br />
4<br />
e<br />
x<br />
1<br />
/( e<br />
x<br />
−1)<br />
2<br />
dx<br />
l l<br />
1<br />
R = R ' −<br />
1 −<br />
2<br />
κ<br />
01<br />
κ<br />
02<br />
l l<br />
2<br />
Can. J. Phys. 37, 334 (1959)
TBR
Boltzmann equation<br />
J. Appl. Phys. 107, 084303 (2010)<br />
Appl. Phys. Lett. 90, 083109 (2007)
Nonequilibrium effects on bulk<br />
κ<br />
2<br />
⎛<br />
⎜<br />
⎜<br />
⎝<br />
L ⎛ 2πl<br />
⎞<br />
= κ<br />
eff<br />
1−<br />
⎜ ⎟ −1<br />
0<br />
2πl<br />
2<br />
⎝ Leff<br />
⎠<br />
2<br />
⎞<br />
⎟<br />
⎟<br />
⎠<br />
J. Appl. Phys. 107, 084303 (2010)<br />
Appl. Phys. Lett. 90, 083109 (2007)
Effective length<br />
L<br />
N −2<br />
N −1<br />
eff<br />
= ( 1− Γ)<br />
L1<br />
+ (1 − Γ)<br />
ΓL2<br />
+ ... + (1 − Γ)<br />
Γ LN-1<br />
+ Γ LN<br />
J. Appl. Phys. 107, 084303 (2010)
Cross plane<br />
κ<br />
κ<br />
CP<br />
CP<br />
=<br />
L<br />
L<br />
κ<br />
1<br />
1<br />
1<br />
+<br />
+<br />
L<br />
L<br />
κ<br />
κ<br />
1<br />
2<br />
2<br />
2<br />
CP<br />
=<br />
+ R<br />
2κ<br />
1+<br />
L +<br />
CP R<br />
L<br />
2<br />
J. Appl. Phys. 107, 084303 (2010)
In plane<br />
κ<br />
IP<br />
=<br />
κ<br />
1<br />
L<br />
L<br />
1<br />
1<br />
+<br />
+<br />
κ<br />
L<br />
2<br />
2<br />
L<br />
2<br />
J. Appl. Phys. 107, 084303 (2010)
SL <strong>effective</strong> <strong>thermal</strong> <strong>conductivity</strong><br />
J. Appl. Phys. 107, 084303 (2010)
SL <strong>effective</strong> <strong>thermal</strong> <strong>conductivity</strong><br />
J. Appl. Phys. 107, 084303 (2010)
Conclusions<br />
• Non-Equilibrium Thermodynamics combined with<br />
TBR models gives a good approximation <strong>for</strong> <strong>thermal</strong><br />
<strong>conductivity</strong> <strong>of</strong> <strong>superlattices</strong><br />
• Obtained <strong>expression</strong>s are simple and analytical
Thank you