Chemical warfare agents containing phosphonate ester bonds are among the most toxic chemicals known to mankind. Recent global military events, such as the conflict and disarmament in Syria, have brought into focus the need to find effective strategies for the rapid destruction of these banned chemicals. Solutions are needed for immediate personal protection (for example, the filtration and catalytic destruction of airborne versions of agents), bulk destruction of chemical weapon stockpiles, protection (via coating) of clothing, equipment and buildings, and containment of agent spills. Solid heterogeneous materials such as modified activated carbon or metal oxides exhibit many desirable characteristics for the destruction of chemical warfare agents. However, low sorptive capacities, low effective active site loadings, deactivation of the active site, slow degradation kinetics, and/or a lack of tailorability offer significant room for improvement in these materials. Here, we report a carefully chosen metal-organic framework (MOF) material featuring high porosity and exceptional chemical stability that is extraordinarily effective for the degradation of nerve agents and their simulants. Experimental and computational evidence points to Lewis-acidic Zr(IV) ions as the active sites and to their superb accessibility as a defining element of their efficacy.

Gas separations with porous materials are economically important and provide a unique challenge to fundamental materials design, as adsorbent properties can be altered to achieve selective gas adsorption. Metal−organic frameworks represent a rapidly expanding new class of porous adsorbents with a large range of possibilities for designing materials with desired functionalities. Given the large number of possible framework structures, quantum mechanical computations can provide useful guidance in prioritizing the synthesis of the most useful materials for a given application. Here, we show that such calculations can predict a new metal− organic framework of potential utility for separation of dinitrogen from methane, a particularly challenging separation of critical value for utilizing natural gas. An open V(II) site incorporated into a metal−organic framework can provide a material with a considerably higher enthalpy of adsorption for dinitrogen than for methane, based on strong selective back bonding with the former but not the latter. ■ INTRODUCTIONCoordination of dinitrogen to transition-metal cations is important both fundamentally and industrially. Dinitrogen is highly inert and generally considered to be a poor ligand. In 1965, however, it was shown that a simple coordination complex, [Ru(NH 3 ) 5 ] 2+ , could reversibly bind N 2 . 1 In subsequent years, a number of dinitrogen−transition-metal complexes have been isolated for metals in varying oxidation states with various coordination numbers. 2,3 These complexes typically feature low-valent, relatively reducing metal cations coordinated to dinitrogen in an end-on binding mode. Activating dinitrogen at a metal center to promote its reduction by hydrogen to ammonia under moderate conditions remains a critical goal for homogeneous catalysis. Somewhat weaker metal−dinitrogen binding, however, may be useful for adsorptive separation of gas mixtures. An example is provided by the need to remove dinitrogen (an omnipresent but noncombustible contaminant) from natural gas or other methane-rich gases. This is an extraordinarily difficult separation based on physical properties alone, as both gases lack a permanent dipole and have similar polarizabilities, boiling points, and kinetic diameters. Although cryogenic distillation is currently utilized for separation of these gases, the cost-and capital-intensive nature of this separation has led to development of a number of competing processes, such as membraneor kinetics-based separations, which generally suffer from low selectivities. 4

Azobenzene undergoes reversible cis<-->trans photoisomerization upon irradiation. Substituents often change the isomerization behavior of azobenzene, but not always in a predictive manner. The synthesis and properties of three azobenzene derivatives, AzoAMP-1, -2, and -3, are reported. AzoAMP-1 (2,2'-bis[N-(2-pyridyl)methyl]diaminoazobenzene), which possesses two aminomethylpyridine groups ortho to the azo group, exhibits minimal trans-->cis photoisomerization and extremely rapid cis-->trans thermal recovery. AzoAMP-1 adopts a planar conformation in the solid state and is much more emissive (Phi(fl) = 0.003) than azobenzene when frozen in a matrix of 1:1 diethylether/ethanol at 77 K. Two strong intramolecular hydrogen bonds between anilino protons and pyridyl and azo nitrogen atoms are responsible for these unusual properties. Computational data predict AzoAMP-1 should not isomerize following S(2)<--S(0) excitation because of the presence of an energy barrier in the S(1) state. When potential energy curves are recalculated with methyl groups in place of anilino protons, the barrier to isomerization disappears. The dimethylated analogue AzoAMP-2 was independently synthesized, and the photoisomerization predicted by calculations was confirmed experimentally. AzoAMP-2, when irradiated at 460 nm, photoisomerizes with a quantum yield of 0.19 and has a much slower rate of thermal isomerization back to the trans form compared to that of AzoAMP-1. Its emission intensity at 77 K is comparable to that of azobenzene. Confirmation that the AzoAMP-1 and -2 retain excited state photochemistry analogous to azobenzene was provided by ultrafast transient absorption spectroscopy of both compounds in the visible spectral region. The isomerization of azobenzene occurs via a concerted inversion mechanism where both aryl rings must adopt a collinear arrangement prior to inversion. The hydrogen bonding in AzoAMP-1 prevents both aryl rings from adopting this conformation. To further probe the mechanism of isomerization, AzoAMP-3, which has only one anilinomethylpyridine substituent for hydrogen bonding, was prepared and characterized. AzoAMP-3 does not isomerize and exhibits emission (Phi(fl) = 0.0008) at 77 K. The hydrogen bonding motif in AzoAMP-1 and AzoAMP-3 provides the first example where inhibiting the concerted inversion pathway in an azobenzene prevents isomerization. These molecules provide important supporting evidence for the spectroscopic and computational studies aimed at elucidating the isomerization mechanism in azobenzene.

Targeted covalent inhibitor drugs require computational methods that go beyond simple molecular‐mechanical force fields in order to model the chemical reactions that occur when they bind to their targets. Here, several semiempirical and density‐functional theory (DFT) methods are assessed for their ability to describe the potential energy surface and reaction energies of the covalent modification of a thiol by an electrophile. Functionals such as PBE and B3LYP fail to predict a stable enolate intermediate. This is largely due to delocalization error, which spuriously stabilizes the prereaction complex, in which excess electron density is transferred from the thiolate to the electrophile. Functionals with a high‐exact exchange component, range‐separated DFT functionals, and variationally optimized exact exchange (i.e., the LC‐B05minV functional) correct this issue to various degrees. The large gradient behavior of the exchange enhancement factor is also found to significantly affect the results, leading to the improved performance of PBE0. While ωB97X‐D and M06‐2X were reasonably accurate, no method provided quantitative accuracy for all three electrophiles, making this a very strenuous test of functional performance. Additionally, one drawback of M06‐2X was that molecular dynamics (MD) simulations using this functional were only stable if a fine integration grid was used. The low‐cost semiempirical methods, PM3, AM1, and PM7, provide a qualitatively correct description of the reaction mechanism, although the energetics is not quantitatively reliable. As a proof of concept, the potential of mean force for the addition of methylthiolate to methylvinyl ketone was calculated using quantum mechanical/molecular mechanical MD in an explicit polarizable aqueous solvent. © 2019 Wiley Periodicals, Inc.

As an intermediate in industrial 2,4,6-trinitrotoluene (TNT) production, 2,4-dinitrotoluene (DNT) is one of the most prevalent impurities in TNT. Its high volatility as compared to TNT makes DNT a telltale sign of TNT explosives, and the electroactivity of its nitro groups lends itself to electrochemical detection as a particularly promising route for DNT sensing. In this work, the electrochemical reduction mechanism of DNT was investigated by cyclic voltammetry. In anhydrous solvents and in the absence of another source of protons, DNT exhibits two well resolved one-electron transfers. The radical anion formed by reduction of DNT is shown to be sufficiently basic to deprotonate the weakly acidic methyl group of still unreacted DNT, giving rise to an intense blue color. In contrast, in the presence of a pH buffer, DNT is readily reduced in acetonitrile to 2,4-bis(N-hydroxylamino)toluene by an irreversible transfer of eight protons and eight electrons. Density functional calculations suggest that the pathway to 2,4-bis(N-hydroxylamino)toluene is thermodynamically more favorable than the formation of aminonitrotoluene. This occurs at a substantially less negative potential than in the absence of protons, which shows that the reduction of DNT in the presence of protons is directly coupled to the protonation of DNT. The enhancement in signal observed for DNT in the presence of protons indicates that the incorporation of a proton source to electrochemical sensing setups will greatly enhance the sensitivity of electroreductive DNT analysis.

We extend the AMOEBA polarizable molecular mechanics force field to the Fe(2+) cation in its singlet, triplet, and quintet spin states. Required parameters are obtained either directly from first principles calculations or optimized so as to reproduce corresponding interaction energy components in a hexaaquo environment derived from quantum mechanical energy decomposition analyses. We assess the importance of the damping of point-dipole polarization at short distance as well as the influence of charge-transfer for metal-water interactions in hydrated Fe(2+); this analysis informs the selection of model systems employed for parametrization. We validate our final Fe(2+) model through comparison of molecular dynamics (MD) simulations to available experimental data for aqueous ferrous ion in its quintet electronic ground state.

Solution-state dynamic nuclear polarization (DNP) is a powerful tool for hyperpolarization and the study of intermolecular interactions in solution.

The behaviour of metal-organic cages upon guest encapsulation can be difficult to elucidate in solution. Paramagnetic metal centres introduce additional dispersion of signals that is useful for characterisation of host-guest complexes in solution using nuclear magnetic resonance (NMR). However, paramagnetic centres also complicate spectral assignment due to line broadening, signal integration error, and large changes in chemical shifts, which can be difficult to assign even for known compounds. Quantum chemical predictions can provide information that greatly facilitates the assignment of NMR signals and identification of species present. Here we explore how the prediction of paramagnetic NMR spectra may be used to gain insight into the spin crossover (SCO) properties of iron(II)-based metal organic coordination cages, specifically examining how the structure of the local metal coordination environment affects SCO. To represent the tetrahedral metal-organic cage, a model system is generated by considering an isolated metal-ion vertex: fac-ML3(2+) (M = Fe(II), Co(II); L = N-phenyl-2-pyridinaldimine). The sensitivity of the (1)H paramagnetic chemical shifts to local coordination environments is assessed and utilised to shed light on spin crossover behaviour in iron complexes. Our data indicate that expansion of the metal coordination sphere must precede any thermal SCO. An attempt to correlate experimental enthalpies of SCO with static properties of bound guests shows that no simple relationship exists, and that effects are likely due to nuanced dynamic response to encapsulation.