Computational Design for Enhanced Hydrogen Storage on the Newly Synthesized 2D Polyaramid via Titanium and Zirconium Decoration

Abstract

2D polyaramid (2DPA) is a porous and polymeric material that has been synthesized recently. Titanium and zirconium decoration over 2DPA increases their affinity for hydrogen substantially, making them suitable for onboard and reversible hydrogen storage, particularly in light-duty vehicles. By decorating a single unit cell of 2DPA with two transition metal (TM) atoms, hydrogen storage of up to 6.422 and 6.792 wt % of H 2 with average binding energies of −0.399 and −0.480 eV is predicted for 2DPA + Ti and 2DPA + Zr, respectively. The binding of Ti and Zr with 2DPA is accompanied by a flow of charge (−1.474e for Ti and −1.696e for Zr) from the TM toward the 2DPA sheet. Further, the interaction between H 2 and the TM may proceed via Kubas interaction between the d orbital of the TM in 2DPA + TM and H 1s orbitals of H 2 , with a net flow of charge from the TM toward H 2 (−0.218e for Ti and −0.391e for Zr). The desorption of H 2 bound to 2DPA + Zr is endothermic (∼0.57 eV) and close in magnitude to the binding energy of the first H 2 (∼−0.544 eV). The 2DPA + TM systems show structural and dynamic stability at high temperatures, as evident from ab initio molecular dynamics simulations and phonon spectra. The movement of TM atoms across the 2DPA sheet to form clusters may be hindered by the considerable barrier energy (∼4.9 eV for Ti). Through these systematic density functional theory simulations, we predict that Ti-and Zr-decorated 2DPA are high-performance hydrogen storage materials and can be explored by experimentalists.

Lithium Functionalization in a Three-Dimensional Graphene Monolith for Enhanced Adsorption–Desorption Hydrogen Storage

“…Since the breakthrough discovery of “ Graphene” , two-dimensional (2D) materials have been successfully studied theoretically and experimentally as potential applications in hydrogen storage, ,, due to their unique structural and physicochemical properties. Regrettably, these pure 2D materials suffer from two significant drawbacks; (i) the gravimetric density of H 2 is fairly lower than the target required by the DoE (<5.5 wt %), and (ii) the hydrogen desorption temperature is considerably lower than room temperature, primarily due to the weak van der Waals interaction between H 2 molecules and the material’s substrate.…”