Abstract

In the present work, an in-depth, qualitative and quantitative description of non-covalent interactions in the hydrogen storage materials LiN(CH3)2BH3 and KN(CH3)2BH3 was performed by means of the charge and energy decomposition method (ETS-NOCV) as well as the Interacting Quantum Atoms (IQA) approach. It was determined that both crystals are stabilized by electrostatically dominated intra- and intermolecular M∙∙∙H–B interactions (M = Li, K). For LiN(CH3)2BH3 the intramolecular charge transfer appeared (B–H→Li) to be more pronounced compared with the corresponding intermolecular contribution. We clarified for the first time, based on the ETS-NOCV and IQA methods, that homopolar BH∙∙∙HB interactions in LiN(CH3)2BH3 can be considered as destabilizing (due to the dominance of repulsion caused by negatively charged borane units), despite the fact that some charge delocalization within BH∙∙∙HB contacts is enforced (which explains H∙∙∙H bond critical points found from the QTAIM method). Interestingly, quite similar (to BH∙∙∙HB) intermolecular homopolar dihydrogen bonds CH∙∙∙HC appared to significantly stabilize both crystals—the ETS-NOCV scheme allowed us to conclude that CH∙∙∙HC interactions are dispersion dominated, however, the electrostatic and σ/σ*(C–H) charge transfer contributions are also important. These interactions appeared to be more pronounced in KN(CH3)2BH3 compared with LiN(CH3)2BH3.

Highlights

  • An increase in energy consumption as well as the environmental harmfulness of current coal or hydrocarbon based fuels has led to intensive search for alternative energy sources [1,2,3]

  • Are for the first time quantitatively described by means of and KN(CH3)2BH3 are for the first time quantitatively described by means of the the charge and energy decomposition method ETS-Natural Orbitals for Chemical Valence (NOCV) as well as the Interacting Quantum Atoms (IQA) approach

  • The intramolecular charge transfer contributing to Li ̈H–B

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Summary

Introduction

An increase in energy consumption as well as the environmental harmfulness of current coal or hydrocarbon based fuels has led to intensive search for alternative energy sources [1,2,3]. For example one can present ammonia borane (NH3 BH3 ) [4,5,6,7,8,9,10]—the attractiveness of this material stems from its high stability, even at higher temperature (the melting point is 104 ̋ C), as well as its large hydrogen storage capacity (19.6 wt% H2 ). It has been demonstrated that the former feature of ammonia borane crystal originates predominantly from the existence of polar dihydrogen bonds N–Hδ ̈ ̈ ̈ ́δ H–B between monomers [11,12,13,14,15,16]. It has been proven that the presence of N–Hδ ̈ ̈ ̈ ́δ H–B as well as other non-covalent interactions determines the stability, but it can facilitate various steps of dehydrogenation [5,6,7,8,11,12,13,14,15,16,17,18,19,20,21,22,23]

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