An Investigation of Boron Nitride Nanomaterial Functionalization
At the Army Research Laboratory
by Kevin Waters
Follow along @ kwaters4.github.io/Presentation/ARL/
"We can accurately predict the interface between biological molecules and nanomaterials in physiological conditions."
Materials with at least one dimension in the sub-micron range.
- Ratio of surface to bulk atoms changes
- Bulk properties are not present at this scale
- Adding one atom changes the properties of the material
- Large configuration spaces to search
- Prediction can be utilized, but caution should be practiced
- Clusters
- Nanoparticles
- Fullerenes
- Nanotubes
- 2D-Materials
A. K. Geim et. al Nature Materials (2007) 6: 183
- Predicted in 1994
- Synthesized in 1995
- Typically considred a wide band gap semiconductor
- Parameters to consider
- Chirality (n,n), (n,0), (n,m)
- Diameter
- Layers
- Excellent chemical and thermal stability
- Semi-ionic bonds (B-N) versus covalent (C-C)
- Interlayer interactions are stronger
- BNNTs are mostly zig-zag, CNTs statistcally equivalent.
- All BNNTs are semi-conducting, CNTs vary based on chirality
- Cytotoxicity still being investigated for BNNTs
Rimola et. al. (2013) PCCP 15:13190
- Carbohydrates
- DNA (Nucleotides)
- Lipids
- Proteins (Amino Acids, Peptides)
- etc.
- Solving the system's electronic wavefunction
- Schrödinger Equation
- Density Functional Theory (DFT)
- Ab Initio Molecular Dynamics (AIMD)
- High Performance Computing Platform
pdb : 3V03 |
Waters et. al. (2017) ACS Omega 2:76
Sainsbury et. al. (2007) JACS 111:12992
Coverage (%) |
Band Gap (eV) |
Binding Energy (eV) |
0 |
4.25 |
|
16 |
3.34 |
-0.74 |
25 |
3.11 |
-0.70 |
50 |
2.25 |
0.72 |
- Supercell : 2B + 4N
- Symmetry : Amm2 (38)
- Lattice Vectors
- Bonds
- N-N : 1.29 Å
- N-B : 1.34 Å
- B-N : 1.50 Å
- Stability : Phonon Spectra
- σI is the stress tensor
- CIJ is the elastic tensor
- ηJ is the stain tensor
N/m |
Graphene1 |
This Work |
BN2 |
This Work |
C11 |
358.1 |
353.7 |
293.2 |
290.5 |
|
C12 |
60.4 |
61.7 |
66.1 |
64.4 |
|
C22 |
|
|
|
|
|
C66 |
148.9 |
144.9 |
113.5 |
113.1 |
|
N/m |
Graphene1 |
BN2 |
BN2 |
C11 |
358.1 |
293.2 |
368.8 |
C12 |
60.4 |
66.1 |
47.2 |
C22 |
|
|
153.3 |
C66 |
148.9 |
113.5 |
58.7 |
Mechanical Properties of Crystalline Poly Ether Ether Ketone (PEEK)
Pisani et. al. (2018) In Prepartation
- The Institute for Ultra-Strong Composites by Computational Design
- NASA Space Technology Research Institute
- Computationally-driven development of CNT-based ultra high strength lightweight structural materials
- Project lead by Dr. Odegard at Michigan Tech.
- Investigating properties of the polymers for future applications
- ReaxxFF testing and validation
- Comparing crystalline data (MD vs. DFT)
- Challenging to model amorphous PEEK with electron approach
(GPa) |
MD |
DFT |
C11 |
140.5 ± 7.31 |
133.3 |
C22 |
4.87 ± 1.56 |
15.5 |
C33 |
7.18 ± 1.34 |
15.3 |
C44 |
0.24 ± 0.16 |
14.0 |
C55 |
3.79 ± 3.00 |
9.0 |
C66 |
3.37 ± 0.36 |
4.8 |
|
MD |
DFT |
ν12 |
0.88 ± 0.24 |
0.38 |
ν13 |
-0.01 ± 0.58 |
-0.33 |
ν23 |
0.50 ± 0.12 |
0.38 |
Gold Deposition on Boron Nitride Nanomaterials
Waters et. al. (2018) In Prepartation
Unpublished work from Bhandari et. al.
- Substrate of h-BN
- vDW Interactions
- Deformation for 3D clusters
- Improve accuracy for the exact exchange integral in PBC (NWChem)
- AIMD studies on the peptide/BNNTs interface in a solvated environment
- Test plane-wave AIMD simulations with O(N) DFT methods
Challenges
- Computation power (Hardware/Software)
- Scaling of theories (CCSD vs. DFT vs. MD)
- Inclusion of all releveant parameters (ions, solution, pH, etc.)
- Asking the right questions
Conclusion
- Laid the foundation for protein BNNT simulations
- Started to investigate functionalized structures
- Building framework for future large scale applications
- Flexibility to look at similar structures (e.g. Polymers)
Acknowledgements
- Ravindra Pandey
- Eric Bylasksa
- Gregory Odegard
- Nabanita Saikia
- Max Seel
- Wil Slough
- Yoke Khin Yap