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Graphene-based Thermal Interface Materials (TIM)

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Title: Graphene-based Thermal Interface Materials (TIM)


1
Graphene-based Thermal Interface Materials (TIM)
  • A proposal submitted to
  • CTRC (Cooling Technologies Research Center)

Principle investigators Yong P. Chen (Physics,
ECE and Birck Nanotechnology Center) Xiulin Ruan
(ME) Tim S Fisher (ME and Birck Nanotechnology
Center) Purdue University
2
Why Graphene
  • Graphene building block
  • for most carbon materials
  • ---incl. graphite and
  • carbon nanotubes(CNT)
  • Recently, carbon materials
  • (incl. both graphite and CNT)
  • investigated as attractive
  • thermal interface material
  • (TIM) motivated by their
  • high thermal conductivity

c
b
a
(discovered 2004)
  • Other advantages of graphene
  • High packing density due to 2D
  • rich shapes/geometry
  • Easily functionalized
  • Possibilities to bond to surface

Graphene extraordinary thermal conductivity
3000-5000 W/mK Nano Lett. 8, 902907, 2008
(highest among materials responsible for the
high thermal conductivity of graphite (ab-plane)
and CNT!
3
Research Objectives
  • Develop high performance TIM based on graphene
  • Approach 1 (focus) Vertically grown (CVD)
    graphene sheets
  • between (and bonded to) substrates
  • Approach 2 (reference) Graphite micro
    platelets/powder
  • between substrates
  • Components
  • material (TIM) design
  • synthesis/fabrication
  • thermal measurements
  • modeling

Some key issues -Bonding of filler material
(graphene) to surface -Adhesion between filler
materials
  • Metrics to Achieve
  • Material thermal conductivity gt 1000 W/mK
  • Interface thermal resistance lt1 mm2K/W

4
Approach 1 Vertically Grown Graphene Sheets by
CVD
  • Microwave plasma enhanced (PE)
  • chemical vapor deposition (CVD) grows
  • vertically aligned graphene sheets
  • No catalyst needed
  • Works on almost any substrate
  • graphene bonded to substrate surface
  • can have very high filling/packing density

Malesevic et al., Nanotechnology2008
Key idea CVD grow vertical graphene between two
substrates as TIM
substrate
graphene
interface
substrate
Carbon PECVD apparatus available in Purdue/Birck
(Fisher)
5
Approach 2 Graphite Platelets, Powders and
Graphene Composites
  • Graphite ab-plane has extraordinary thermal
    conductivity (due to graphene thermal
    conductivity)
  • Make graphite (highly ordered pyrolytic
    graphite) platelets with thin (vertical)
    dimension along ab
  • Fill such graphite platelets as filler material
    between two substrates as TIM
  • Alternative graphite powders (a fraction with
    vertical along ab)
  • low cost, low tech, field-applicable
  • Will investigate geometric factors (size, aspect
    ratio etc) of filler blocks
  • Will investigate various bonding glues/epoxy to
    promote adhesion between fillers and to the
  • substrate surface
  • This is a reference approach that will be
    compared with the CVD grown graphene based TIM
  • to investigate roles of filler materials and
    interface bonding
  • Will also investigate graphene composites

(graphene-polysterene composite, courtesy
D.Dikin, NWU)
6
Measurement Methods
  • Well established methods developed at Purdue
  • for thermal conductivity/interface thermal
    resistance measurements, for example
  • Electrical
  • eg., 3-omega Hu et al., J. Heat Transfer 128,
    1109 (2006)
  • Z. Huang et al., presentation at
    CTRC 10/28/08
  • Optical
  • eg., photoacoustic Cola et al., J. Appl. Phys.
    101, 054303 (2006)
  • Photoreflectance

7
A General Molecular Dynamics Tool for Thermal
Conductance Prediction
  • The tool is based on LAMMPS to perform
    non-equilibrium molecular dynamics simulations
  • Parallel simulation
  • Various types of interatomic potentials
    incorporated
  • 1D, 2D, or 3D arbitrary simulation geometry
  • Easy to extend with new features and
    functionality

8
Thermal Conductivity Prediction of Graphene
  • Non-equilibrium molecular dynamics simulations
  • Impose a heat flux and calculate the temperature
    gradient, so the thermal conductivity is derived
    from Fourier law.

Fourier Law
  • T. Chonan and S. Katayama, J. Phys. Soc. Japn.
  • graphene nanoribbon calculated k1500W/mK
  • (take thickness 0.35nm)

9
Thermal Conductance Prediction of the Graphene
Based TIM
  • Development of the interatomic potentials between
    the carbon atoms and the substrate atoms
  • Non-equilibrium molecular dynamics to calculate
    the thermal conductance of the TIM.
  • Atomistic Greens function will also be used to
    calculate the phonon transmission, and the
    results will be compared to the MD simulations.

10
An interesting MD example thermal rectification
in asymmetric graphene nanoribbon
Rectification factor 3! (largest reported so far)
Jiuning Hu et al., in preparation (2008)
11
Deliverables/Benefits
  • Optimized recipes and procedures to fabricate
    graphene based thermal interface materials.
  • Experimentally validated software simulation tool
    to predict the performance of thermal interface
    materials.

12
Budget and Program Plan
  • 2 years 01/2009-12/2010
  • Each year 45K include
  • 1.5 student support, leveraged by fellowship and
    TA to support 2 students on this project
  • 5000 materials and supplies
  • Student 1 will work on material fabrication and
    thermal measurements
  • Student 2 will develop simulation tool and data
    analysis
  • 1 ECE and 1 ME grad students have been identified
    and ready to perform this research
  • Start TRL3, aim TRL5 at end of program
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