N2-selective metal membranes could be used
to couple
the extraction of N2 from flue gas and NH3 synthesis
within a single membrane reactor. The larger interstitial spaces of
BCC metals make them attractive for fast permeation of the large N
atom. The caveat is that N permeabilities reported thus far for pure
BCC metals (e.g., V, Cr, Fe, Mo, and W) are insufficient for practical
application. However, practical permeabilities could be achieved by
alloying these metals. Here, we use density functional theory (DFT)
to study how alloying V, a metal with high N solubility but low N
diffusivity, with Fe and Cr impacts the dissociation, dissolution,
and diffusion of nitrogen. Although N binding at vacancies was studied,
binding at these defects was not particularly strong compared to regular
interstitial sites, and thus, vacancies may not significantly affect
solubility. The alloys present two types of interstitial octahedral
(o) sites: V-rich (o1) and V-depleted
(o2). Nitrogen binding strength correlates with the
number of V nearest-neighbors; hence, binding in o1 sites is on average 1 eV stronger than in o2 sites.
Ab initio thermodynamics suggests that this combination of strong
and weak binding sites mitigates the reduction in solubility expected
from the alloying (at least at relevant operating conditions). However,
the heterogeneity of the interstitial sites generally leads to higher
energy barriers for N hopping than those encountered in pure V (1.24
eV). The exception to this observation was the V0.25Fe0.75 alloy (1.01 eV). Based on our calculations, at 673 K and
5 bar (N2 pressure), N solubility and diffusivity in V0.25Fe0.75 would be ∼3 times smaller and
∼53 times larger than pure V, respectively. According to the
solution–diffusion model, these findings indicate that an ∼18-fold
higher permeability would be expected for V0.25Fe0.75 relative to V. Permeability is expected to be controlled by bulk
diffusion rather than by surface processes, as in all alloys, we find
the energy barrier for N2 dissociation at the alloy surface
to be lower than the barrier for bulk diffusion in the same alloy.