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Boltzmann Transport Equation - COMSOL.com

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Fourier <strong>Equation</strong> (FE)<br />

• For last two centuries, heat conduction has been modeled by Fourier Eq (FE).<br />

∂T<br />

– Conservation of energy: ρc = −∇ ⋅q<br />

∂t<br />

Diffusive<br />

– Fourier’s linear approximation of heat flux: q = −k∇T L >> Λ T<br />

‣<br />

T 2<br />

1 ∂<br />

= ∇<br />

2 T<br />

α ∂t<br />

x<br />

• Parabolic equation —> Diffusive nature of heat transport. T 1<br />

• Heat is effectively transferred between localized regions through sufficient<br />

scattering events of phonons within medium.<br />

• Does not hold when number of scattering is negligible.<br />

– e.g., mean free path ~ device size (chip-package level).<br />

– Boundary scattering at interfaces causing thermal resistance.<br />

• Admits infinite speed of heat transport —> Contradict with theory of relativity.<br />

L<br />

‣ Fourier <strong>Equation</strong> cannot be used for small time and spatial scales.<br />

3

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