roy downs university of arkansas faculty mentor: dr. joseph j. rencis graduate student mentor:...
TRANSCRIPT
Roy Downs University of Arkansas
Faculty Mentor: Dr. Joseph J. RencisGraduate Student Mentor: Sachin Terdalkar
Nano-indentation of Graphene Sheet using
Molecular Dynamic Simulation
Monolayer Structure of Carbon Atoms
Hexagonal Shape Lattice
Characteristics Very Strong Highly Conductive High Opacity
Graphene Sheet
http://en.wikipedia.org/wiki/File:Graphene_xyz.jpg
• Nano-scale Electronics
• Ultracapacitors
• Pressure Sensors
• Nano Resonators
Potential Applications
[Freitag, M., Nature Nanotechnology 2008]
Graphene Transistor
Experimental Measurement of Mechanical Properties
Mechanical Properties: Project Focuso Young’s Modulus (measured average E=1.0
TPa)o Intrinsic Strength (measured sint=130 GPa)
Indentation Experiment of Graphene on Silicon
Substratehttp://www.sciencemag.org/
Silicon Substrat
eGraphe
ne Sheet AFM Measured E varies
from 0.9 to 1.2 TPa
Atomic Force Microscope
Tip
F - applied force - pretension in graphene sheet - diameter of graphene sheet - indentation depth - Young’s modulus - dimensionless constant
v – Poisson’s ratio varied values of and to fit
the curve in experimental data
Analytical Solution
3322
0
aaqE
aaF DD
D20
DE 2
q
a
216.015.005.1/1 vvq
DE 2 D20
Atoms are assumed lumped point masses
Interaction through Inter-atomic Potential
Atomic position from numerical integration of equations of motion
Molecular Dynamics Simulation
F = ma
http://en.wikipedia.org/wiki/File:Argon_dimer_potential_and_Lennard-
Jones.png
Inte
racti
on e
nerg
y (e
V)
Using MD SimulationsGenerate Load-indentation CurveDetermine Young’s Modulus
Goals
http://www.physorg.com/news135959004.html
Graphene Sheet
Indenter
Monolayer of Graphene SheetLAMMPS - http://lammps.sandia.gov.52873 AtomsRed Atoms Fixed – Outer Diameter Thickness
15 Å Green Atoms Free - Coupled to the External
BathIndenter - 150Å Diameter AIREBO Potential for C-C Interaction
MD Simulation Model
Rigid Indenter
Mobile AtomsFixed Atoms
Stretched with Very Small Velocity to Produce an Infinitesimal Longitudinal and Lateral Strain
Experiment Poisson’s Ratio – 0.165MD Simulation Poisson’s Ratio – 0.166
Calculation of Poisson’s Ratio
y1 = 175.7Å y2
x1=186.3Åx2
Initial Position(t=0; vx = 0)Final Position(t>0)
(vx =0.5 Å/ps)
x
y
x
y
StrainalLongitudin
StrainLateralv
100Å Indenter Diameter 130Å Indenter Diameter
E=1.07 TPa E=1.13 TPa
Varying Diameter of Indenter
3
3220
aaqE
aaF DD AFM Experimentally
Measured E varies from 0.9 to 1.2 TPa
nm.
EE
D
335
2
150Å Indenter Diameter 200Å Indenter Diameter
E=1.18 TPa E=1.28 TPa
Varying Diameter of Indenter
3
3220
aaqE
aaF DD AFM Experimentally
Measured E varies from 0.9 to 1.2 TPanm335.
EE
2D
150Å Indenter Diameter 150Å Indenter Diameter
5Å Eccentricity E=1.17 TPa 10Å Eccentricity E=1.16TPa
Eccentric Indenter
AFM Experimentally Measured
E varies from 0.9 to 1.2 TPanm335.
EE
2D
3
3220
aaqE
aaF DD
MD simulation Compared to Analytical Solution
Indenter SizeIncrease Indenter Diameter -> Increased
Young’s ModulusIndenter Contact Area Affects Measured Value
of Young’s ModulusEccentric Indenter
Does not affect measured value of Young’s modulus
Conclusion
Determine Interaction Between Silicon Substrate and Graphene Sheet
Use MD Simulations
Stone-Wales Defect in Graphene Sheet
Future Work
Silicon Substrat
eGraphene
Sheet