posted on 2021-09-13, 11:41authored byZongtang Fang, Lan Li, David A. Dixon, Rebecca R. Fushimi, Eric J. Dufek
Plane-wave
density
functional theory has been used to study oxygen
adsorption on graphene, graphite, and (12,0) zigzag single-walled
carbon nanotubes with and without Stone–Wales (SW) and single-vacancy
(SV) defects to understand the role of defects on carbonaceous material
reactivity. Atomic oxygen adsorption leads to the formation of an
epoxide on defect-free graphene and graphite and an ether on the exterior
wall of carbon nanotubes and SW-defected materials. O2 chemisorption
is endothermic on defect-free graphene and graphite and slightly exothermic
on defect-free nanotubes. O2 chemisorption energies are
predicted to be −1.1 to −1.4 eV on an SW defect and
−6.0 to −8.0 eV on an SV defect. An SW defect lowers
the energy barriers by 0.90 and 0.50 eV for O2 chemisorption
on graphene and nanotubes, respectively. The formation of a C–O–O–C
group is important for O2 dissociation on defect-free and
SW-defected materials. The energy barrier is less than 0.30 eV on
an SV defect. The more reactive SW defect toward O adsorption on graphene
is mostly due to the strained defective carbon atoms being able to
donate more electrons to an O to form an ether. The larger 2s character
in the hybrid orbitals in an ether than in an epoxide makes the ether
C–O bond stronger. Stronger C–O binding on an SW-defective
carbon nanotube than on a defect-free nanotube is in part due to more
flexibility of the defect to release the epoxide ring strain to form
an ether.