%0 Journal Article
%T Modeling Enhanced Adsorption of Explosive Molecules on a Hydroxylated Graphene Pore
%A Ronald Scott Holt
%A Thomas R. Rybolt
%J Graphene
%P 1-18
%@ 2169-3471
%D 2019
%I Scientific Research Publishing
%R 10.4236/graphene.2019.81001
%X The possibility of a graphene bilayer nanosensor for the detection of explosive molecules was modeled using computational chemistry. A pore was designed on a graphene bilayer structure with three strategically placed perimeter hydroxyl (OH) groups built around the edge of an indented, two-dimensional hexagonal pore. This hydroxylated pore and models of various explosive molecules were optimized using MM2 molecular mechanics parameters. Values were calculated for the molecule-surface interaction energy (binding energy), E, for 22 explosive molecules on a flat graphene bilayer and on the specially designed hydroxylated pore within the bilayer. The molecule-surface binding energy for trinitrotoluene (TNT) increased from 17.9 kcal/mol on the flat graphene bilayer to 42.3 kcal/mol on the hydroxylated pore. Due to the common functionality of nitro groups that exist on many explosive molecules, the other explosive molecules studied gave similar enhancements based on the specific hydrogen bonding interactions formed within the pore. Each of the 22 explosive adsorbate molecules showed increased molecule-surface interaction on the bilayer hydroxylated pore as compared to the flat bilayer. For the 22 molecules, the average E for the flat graphite surface was 15.8 kcal/mol and for the hydroxylated pore E was 33.8 kcal/mol. An enhancement of adsorption should make a detection device more sensitive. Nanosensors based on a modified graphene surface may be useful for detecting extremely low concentrations of explosive molecules or explosive signature molecules.
%K Molecular Mechanics
%K Explosives
%K Molecule-Surface Binding Energy
%K Hydroxylated Graphene Pore
%K Graphene Bilayer
%K Enhanced Adsorption for Explosives
%U http://www.scirp.org/journal/PaperInformation.aspx?PaperID=94577