Davisson-Germer Prize Talk: Hydrogen storage in nanoporous materials
COFFEE_KLATCH · Invited
Abstract
To develop a hydrogen-based energy technology, several classes of materials are being considered to achieve the DOE targets for gravimetric and volumetric hydrogen densities for hydrogen storage, including liquids (e.g. ammonium borohydrides), clathrate structures, complex metal hydrides, nanostructured (e.g. carbon) an nanoporous materials. Fundamental studies are necessary to determine the ultimate hydrogen capacity of each system. Nanoporous Metal-organic Framework (MOF) materials are promising candidates for hydrogen storage because the chemical nature and size of their unit cell can be tailored to weakly attract and incorporate H$_{2}$ molecules, with good volumetric and mass density. In this talk, we consider the structure M$_{2}$(BDC)$_{2}$(TED), where M is a metal atom (Zn, Ni, Cu), BDC is benzenedicarboxylate and TED triethylenediamine, to determine the location and interaction of H$_{2}$ molecules within the MOF. These compounds are isostructural and crystallize in the tetragonal phase (space group P4/ncc), they construct 3D porous structures with relatively large pore size ($\sim $7-8 A\r{ }), pore volume ($\sim $0.63-0.84 cc/g) and BET surface area ($\sim $1500-1900 m$^{2}$/g). At high pressures (300-800 psi), the perturbation of the H-H stretching mode can be measured with IR absorption spectroscopy, showing a 35 cm$^{-1}$ redshift from the unperturbed ortho (4155 cm$^{-1}$ ) and para (4161 cm$^{-1}$ ) frequencies. Using a newly developed non empirical van der Waals DFT method vdW-DFT),\footnote{J.Y. Lee, D.H. Olson, L. Pan, T.J. Emge, J. Li, Adv. Func. Mater. 17, 1255 (2007)} it can be shown that the locus of the deepest H$_{2}$ binding positions lies within to types of narrow channels. The energies of the most stable binding sites, as well as the number of such binding sites, are consistent with the values obtained from experimental adsorption isotherms, and heat of adsorption) data.\footnote{M. Dion, H. Ryberg, E. Schroder, D. C. Langreth, B.I. Lundqvist, Phys. Rev. Lett. 92, 246401 (2004).} Importantly, the calculated shift of the H-H stretch is $\sim $-30 cm$^{-1}$ at the strongest binding points of the two channels, suggesting that the combination of IR and vdW-DFT gives a consistent and accurate picture of H$_{2}$ binding in MOF structures. These methods can therefore provide the fundamental information necessary to guide synthesis for improving H$_{2}$ uptake and release.
–
Authors
-
Yves J. Chabal
University of Texas at Dallas, UT Dallas