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Size effect on thermal conductivity of thin films. Guihua Tang , Yue Zhao, Guangxin Zhai, Zengyao Li, Wenquan Tao School of Energy & Power Engineering, Xi’an Jiaotong University, China. 1. Background. 2. Local mean free path method. 3.1. 3. 3.2. 4. 4. Outline.

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size effect on thermal conductivity of thin films

Size effect on thermal conductivity of thin films

Guihua Tang, Yue Zhao, Guangxin Zhai, Zengyao Li, Wenquan Tao

School of Energy & Power Engineering,

Xi’an Jiaotong University, China

slide2

1

Background

2

Local mean free path method

3.1

3

3.2

4

4

Outline

Results 1: Local thermal conductivity distribution

Results 2:Overall thermal conductivity

Conclusions

slide3

1. Background

  • Boundary or interface scattering becomes important when the characteristic length (film thickness, wire diameter) is comparable with the mean free path.
  • The thermal conductivity (as well as other transport coefficients, viscosity) becomes size dependent.
  • Numerous important applications of nanoscale thermal conduction (electronic devices cooling, thermal insulator, thermalelectric conversion, etc.)
slide4

Z

y

The Phonon Gas

X

is the lattice volumetric specific heat;

is the average speed of phonons;

is the phonon mean free path.

  • Specific heat of solid: Lattice vibration in solids.

Harmonic oscillator model of an atom

  • Conduction in insulatorsis dominated by lattice waves or phonons.
  • Simple expression of thermal conductivity based on the kinetic theory
slide5

is bulk mean free path

Apply the Matthiessen’s rule

  • Classical size effect based ongeometric consideration (1)
  • In the ballistic transport limit, L<<Lb, the MFP is L
  • L>>Lb, the MFP is the bulk mean free path Lb
  • Intermediate region:
slide6

L

A thin film for paths originated from the boundary surface

(m≈3)

Simple interpolation between the two expressions

  • Classical size effect based ongeometric consideration (2)
  • When L<<Lb, assuming that all the energy carriers originate from the boundary surface
  • L>>Lb, the MFP is the bulk mean free path Lb
slide7

L

(m≈3)

A thin film for paths originated from the centre

Interpolation

  • Classical size effect based ongeometric consideration (3)
  • The direction of transport was not considered and the anisotropic feature cannot be captured
  • Filk and Tien employed a weighted average of the mean free path components in the parallel and normal directions of a thin film
slide8

L

Interpolation

(m≈4/3)

  • Classical size effect based ongeometric consideration (4)

A thin circular wire for paths originated from the centre

slide9

Thin

Film

Thin

Wire

p is the probability of specular scattering on the boundary

  • Classical size effect based onBoltzmann Transport Equation (BTE)
  • The relaxation time approximation was adopted.
  • The distribution function was assumed to be not too far away from equilibrium.
slide10

For a thin film:

2. Local mean free path method

  • For an unbounded phonon gas, the probability of a phonon gas can travel between two consecutive collisions with other phonons at location x and x+dx would be of the form:

The probability of a phonon gas having a free path between x and x+dx

  • When the gas is bounded, a number of phonons will be terminated by the boundary, thus effective MFP < Lb
slide13

3. Results

Local thermal conductivity distribution in a semi-infinitefilm

slide14

L

Local thermal conductivity distribution in a thin film

slide16

4. Conclusions

  • An equation to calculate the size-dependent film thermal conductivity has been derived. No Matthiessen’s rule; No interpolation
  • Local thermal conductivity distribution in the thin film has been obtained.
  • The present solution seems to overpredicts reduction in thermal conductivity compared to the data in references when Knudsen number is larger than 1.
  • More cases are needed for further validation and extension to complicated geometric structures.
slide17

Thanks for

your attention!

09/07/2010

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