Elsevier

Chemical Physics Letters

Volume 759, 16 November 2020, 137946
Chemical Physics Letters

Research paper
Counterintuitive bond paths: An intriguing case of the C(NO2)3- ion

https://doi.org/10.1016/j.cplett.2020.137946Get rights and content

Highlights

  • The O⋯O contacts in C(NO2)3- are destabilizing.

  • A bond path does not mean stabilizing nor attractive interaction.

  • The benefit of the rotation of the nitro groups is in the C–N bonds.

Abstract

Based on the finding that, like the planar form, also the relaxed form of the C(NO2)3- ion features OO bond paths between adjacent nitro groups, Luaña et al. [J. Phys. Chem. B 107 (2003) 4912] have announced that these interactions are stabilizing. However, it will be shown that the presence of a bond path strongly depends on the computational model used and that these interactions are destabilizing. Thus the presence of a bond path between a pair of atoms is not evidence of attractive interaction between these atoms. The benefit of the partial rotation of the nitro groups during relaxation of the planar form is also given.

Introduction

Despite the solid mathematical and physical foundations, the Quantum Theory of Atoms in Molecules (QTAIM) [1] proposed by Bader caused a lot of confusion in theories of chemical bond and intermolecular interactions, which seems to occasionally also manifest itself nowadays. This confusion was basically caused by one sentence resulting from this theory, which states that, for any pair of atoms, the simultaneous presence of a bond path and a bond critical point is a necessary and, moreover, sufficient condition to declare that these atoms are bonded to one another [1]. The significance of this statement is revealed in obtaining the ability to easily find chemical bonds using molecular graphs, i.e. diagrams displaying spatial distribution of bond paths and their critical points. The fact that in many simple cases the molecular graph is a mapping of a molecular structural formula [2] has strengthened the belief that a bond path can indeed be indentified with an appropriate chemical bond [3]. This belief has given great popularity and almost uncritical confidence in QTAIM. Much later, however, Bader, in a rather subtle way based on English terminology, tried to significantly loosen the described alignment of a chemical bond with a bond path [4], [5].

Since a chemical bond should be a stabilizing, i.e. binding, interaction, it might have seemed obvious that the presence of a bond path between any pair of atoms means their local stabilization. Nevertheless, Cioslowski, Mixon and Edwards [6], [7], [8] have initiated a long-lasting [9], [10], [11], [12], [13], [14], [15], [16], [17], [18], [19], [20], [21], [22], [23], [24], [25], [26], [27], [28], [29], [30], [31], [32], [33], [34], [35] discussion on whether equating a bond path with a stabilizing, i.e. attractive, interaction is actually correct. Namely, they have shown that the simultaneous presence of a bond path and a corresponding bond critical point is not necessarily equivalent to a stabilizing effect, and quite the opposite, this presence may result from a repulsive interaction between atoms [6], [7], [8].

In addition to somewhat exotic but very important endohedral systems [10], [11], [12], [13], bond paths for XY interactions, which are likely to be destabilizing, also occur between a whole lot of combinations of X and Y atom pairs (where X and Y are e.g. H, O, S, F, Cl, Br, I, etc.) in many smaller or larger molecular systems [9], [10], [11], [12], [13], [14], [15], [16], [17], [18], [19], [20], [21], [22], [23], [24], [25], [26], [27], [28], [29], [30], [31], [32], [33], [34], [35]. Moreover, which may seem strange at first, most of these interactions relate to closely spaced highly electronegative atoms with the same signs (especially negative) of atomic charges, where strong interatomic repulsion would rather be expected [9], [10], [11], [12], [13], [14], [15], [17], [18], [19], [20], [21], [22], [23], [24], [25], [26], [27], [28], [29], [30], [31], [32], [33], [34], [35], [36]. For this reason, this type of bond path may be called counterintuitive [35]. Importantly, it has been shown that many such XY counterintuitive interactions are indeed destabilizing [7], [8], [9], [10], [11], [19], [20], [23], [24], [25], [26], [27], [28], [33], [34], [35].

There are certainly a lot of examples with a counterintuitive bond path. For a more comprehensive analysis of various cases, see Refs. [34], [35] . In this article, I will discuss the OO bond paths in the C(NO2)3- anion. Topology of the electron density distribution of the C(NO2)3- ion was first studied by Cioslowski et al. [6] and then by Luaña et al. [17]. Intriguingly, while the former group of authors have reported that the OO bond paths between adjacent nitro groups are result of repulsion between close atoms, the latter one has considered this interaction as stabilizing. Moreover, as the argument against the idea of locally repulsive OO interactions in this ion suggested by Cioslowski et al. [6], Luaña et al. have argued that “the “steric crowding” is eliminated in the nonplanar optimal geometry of C(NO2)3- by the rotation of the NO2 groups around the C-N axes, but the fact is that the Osingle bondO bonds do not disappear by this relaxation of the symmetry.” [17].

The purpose of this article is to show that for twisted, i.e. fully optimized ion, the OO bond paths between adjacent nitro groups disappear in fact if only a better computational model (i.e. the level of theory) is used. Then I will show that these OO interactions are actually destabilizing and the cause of twisting of the nitro groups during relaxation of geometry of the planar form of the C(NO2)3- ion will be given. I will also discuss the most reliable molecular graphs of C(NO2)3- in the context of the Poincaré-Hopf relationship.

Section snippets

Methodology

At the beginning, optimizations of both the planar and twisted structures of the C(NO2)3- ion were performed. Frequency calculations confirmed that the former structure corresponds to a transition state, whereas the latter one is a real minumum on the potential energy hypersurface. These calculations were made using 541 different levels of theory, which were combinations of 5 methods

Results and discussion

As mentioned in Introduction, the artificial planar form of the C(NO2)3- ion was an important example of a system featuring the presence of counterintuitive OO bond paths. Cioslowski et al. [6] have concluded that these bond paths result from repulsive interactions between closely spaced oxygen atoms. As an argument against the idea of the repulsive OO interaction suggested by Cioslowski et al., Luaña et al. [17] have stated that the OO bond paths are still present in the twisted i.e. fully

Conclusions

Almost from the very beginning of QTAIM introduced by Bader, there is an interesting discussion on whether the presence of a bond path between any pair of atoms really means a stabilizing interaction between these atoms. The basic object of this discussion are the so-called counterintuitive bond paths that occur between atoms showing the same sign of atomic charge, especially negative, such as OO. One example of such opposing views on the repulsive/attractive role of OO contacts was related

Additional remarks

Although one of the Reviewers pointed out that the OO bond path provides a scaffold for conformational changes, which is of particular importance in the context of hydrogen bonds in (H2O)5 water aggregates, where it is more efficient to form or break a HO hydrogen bond via an OO interaction [50], it does not change the fact the OO interaction is destabilizing, i.e. repulsive, as is shown by the positive value of the interatomic interaction energy (EintOO) obtained using the IQA method – so

CRediT authorship contribution statement

Mirosław Jabłoński: Conceptualization, Data curation, Formal analysis, Investigation, Methodology, Supervision, Validation, Visualization, Writing - original draft, Writing - review & editing.

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

References (50)

  • J. Cioslowski et al.

    Weak bonds in the topological theory of atoms in molecules

    J. Am. Chem. Soc.

    (1991)
  • J. Cioslowski et al.

    Topological properties of electron density in search of steric interactions in molecules: electronic structure calculations on ortho-substituted biphenyls

    J. Am. Chem. Soc.

    (1992)
  • J. Cioslowski et al.

    Universality among topological properties of electron density associated with the hydrogen–hydrogen nonbonding interactions

    Can. J. Chem.

    (1992)
  • J. Cioslowski et al.

    Steric overcrowding in perhalogenated cyclohexanes, dodecahedranes, and [60]fulleranes

    J. Am. Chem. Soc.

    (1995)
  • A. Haaland et al.

    Topological analysis of electron densities: is the presence of an atomic interaction line in an equilibrium geometry a sufficient condition for the existence of a chemical bond?

    Chem. Eur. J.

    (2004)
  • T. Strenalyuk et al.

    Chemical bonding in the inclusion complex of He in adamantane (He@adam): the origin of the barrier to dissociation

    Chem. Eur. J.

    (2008)
  • E. Cerpa et al.

    The implications of symmetry of the external potential on bond paths

    Chem. Eur. J.

    (2008)
  • E. Cerpa et al.

    Influence of endohedral confinement on the electronic interaction between He atoms: a He2@C20H20 case study

    Chem. Eur. J.

    (2009)
  • R.G.A. Bone et al.

    Identifying and analyzing intermolecular bonding interactions in van der Waals molecules

    J. Phys. Chem.

    (1996)
  • C.F. Matta et al.

    Hydrogen – hydrogen bonding: a stabilizing interaction in molecules and crystals

    Chem. Eur. J.

    (2003)
  • V. Luaña et al.

    Ions in crystals: the topology of the electron density in ionic materials. 4. The danburite (CaB2Si2O8) case and the occurrence of oxide-oxide bond paths in crystals

    J. Phys. Chem. B

    (2003)
  • C.F. Matta et al.

    Characterization of a closed-shell fluorine-fluorine bonding interaction in aromatic compounds on the basis of the electron density

    J. Phys. Chem. A

    (2005)
  • J. Poater et al.

    Hydrogen-hydrogen bonding in planar biphenyl, predicted by atoms-in-molecules theory, does not exist

    Chem. Eur. J.

    (2006)
  • J. Poater et al.

    A model of the chemical bond must be rooted in quantum mechanics, provide insight, and possess predictive power

    Chem. Eur. J.

    (2006)
  • A.M. Pendás et al.

    Bond paths as privileged exchange channels

    Chem. Eur. J.

    (2007)
  • Cited by (0)

    View full text