Aurelia
Falcicchio‡
a,
Sten O.
Nilsson Lill‡
b,
Filippo M.
Perna
c,
Antonio
Salomone
c,
Donato I.
Coppi
c,
Corrado
Cuocci
a,
Dietmar
Stalke
d and
Vito
Capriati
*c
aIstituto di Cristallografia (IC-CNR), Via Amendola 122/o, I-70125 Bari, Italy
bPharmaceutical Innovation, Pharmaceutical Development, AstraZeneca, Pepparedsleden 1, SE-431 83, Mölndal, Sweden
cDipartimento di Farmacia-Scienze del Farmaco, Università di Bari “Aldo Moro”, Consorzio C.I.N.M.P.I.S., Via E. Orabona 4, I-70125, Bari, Italy. E-mail: vito.capriati@uniba.it
dInstitut für Anorganische Chemie, Universität Göttingen, Tammannstraße 4, D-37077, Göttingen, Germany
First published on 26th June 2015
The first structure of an aromatic bis(trifluoroborate) dipotassium salt, elucidated by the combination of crystallography, DFT calculations, topological and non-covalent interaction analysis, discloses a 3D network undergoing spontaneous self-assembly thanks to the massive participation of weak intra- and intermolecular interactions for which fluorine atoms proved to play a leading role.
However, despite the exponential growth of papers dedicated to potassium organotrifluoroborates in the last 10 years, few investigators have, to date, concentrated their research on the structures of such salts.6 The few X-ray structure determinations reported so far for compounds containing a benzene ring carrying at least one –BF3K group7 reveal the singular and unique feature of each organotrifluoroborate salt in which large polarizable cations such as K+ (which are significantly better charge-delocalizing than Li+) permit extended crystal lattices to form because of their multihapto coordinations.8 Such molecular structures are often held together by weaker coordinations (e.g., C–H⋯π, K⋯π and π–π interactions) and, sometimes, also by long-range electrostatic forces. All these interactions contribute to define the final architecture of the packing.
This self-assembly aspect of organotrifluoroborates is surely amazing and worth investigating because the peculiar nature of each salt may promote self-organization and thus the obtainment of functional supramolecular architectures with potential interest in many fields (e.g., materials science, catalysis, sensing and separations) as has recently been ascertained in the case of boronic acids, which have been shown to undergo spontaneous supramolecular assembly either with themselves or with other N-donor compounds.9 Aromatic and heteroaromatic bis- and poly(trifluoroborate) compounds have also been successfully employed in the manufacture of novel conjugated polymers with excellent and interesting electron-transport properties.10 Thus, the design and synthesis of novel polyfunctional aromatic compounds carrying more than one trifluoroborate group onto the aromatic core is fascinating and challenging both from a crystallographic and a synthetic perspective in order to chemoselectively replace them in multistep organic synthesis and to obtain new functional structural motifs.
Recently, we have described the preparation of bifunctional dipotassium phenylene-1,4-bis(trifluoroborate) 2 from the corresponding commercially available bis(boronic acid) 1 (Scheme 1) and its successful employment in one-pot double Suzuki–Miyaura coupling reactions for the obtainment of conjugated tri(hetero)aryl derivatives.11
In this paper, we present the first structural investigations on such a salt (2) which provide detailed insight on the presence of an impressive multitude of weak inter- and intramolecular interactions responsible for its self-assembly into a new 3D network.
Bis-trifluoroborate 2, directly obtained as a white free-flowing powder in 92% yield, has been crystallized at room temperature by slow evaporation from a solution of 2:1 acetone/H2O (in ratio 2:1) and colourless needles (mp 342 °C) have been collected. Bis(trifluoroborate) 2, crystallizes in a tetragonal crystal system, in the space group I4l/acd with the cell parameters a = 17.597(9) Å and c = 40.203(9) Å. The asymmetric unit consists of 1.5 independent molecules of C6H4B2F6, 5 K atoms (one of them at the general position, and the rest at special positions with a site occupancy factor of 0.5) and half a molecule of H2O. A view of the refined crystal structure is shown in Fig. 1 where short K⋯F and K⋯O contacts are distinguishable. Of note, the H atom of the 0.5 H2O molecule points towards the benzene ring, the distance between the centroid of the aromatic ring and the H atom (labelled as H100) being 2.475 Å, thereby suggesting the presence of an aromatic OH⋯π interaction (vide infra).12
The C–C bond lengths of the aromatic ring vary from 1.383(4) Å up to 1.397(4) Å and are thus consistent with π delocalization; the ring is, indeed, essentially planar. The B–F bond lengths range from 1.391(4) Å for B3–F9 to 1.447(3) Å for B1–F2 (Table S1, ESI†) and are in agreement with the values reported in the literature.7c,f All the three F atoms belonging to BF3 groups lie out of the plane of the aromatic ring.§ Analogous to what has been reported for other organotrifluoroborates,7f,10b,c the coordination geometry around all K+ cations is irregular and cannot be conveniently described by any polyhedron,13 K⋯F contacts ranging from 2.621(2) Å (K4⋯F8) to 3.382(3) Å (K3⋯F9). In particular, cations K1, K2 and K3 all have ten short contacts to F atoms (most of them less than 3.0 Å, see the ESI†), and two slightly longer contacts to B atoms (Table S1, ESI†). The environment of the K4 cation, which is depicted in Fig. 2, shows eight short contacts to F atoms in the range 2.621(2) Å–3.041(2) Å. In the case of a K5 cation, four interactions with F atoms less than 3.0 Å, one to oxygen 2.7247(17) Å and two distances to carbons C5 and C8 longer than 3.3 Å are present, instead.
Fig. 2 The environment of K4 cation. Symmetry codes: (i) −x + 1, −y + ½, z; (ii) −x + 1, −y, −z; (iii) x, y + ½, −z; (iv) −y + ¾, x − ¼, −z + ¼; (v) y + ¼, −x + ¾, −z + ¼. |
Fig. 3 depicts the packing of the title compound revealing the presence of K cation layers bridged by C6H4B2F6 and H2O molecules via K⋯F, K⋯O, OH⋯π and K⋯aryl interactions. Thus, despite its apparent structural and spectroscopic simplicity,¶ the overall 3D network of the salt 2 is made up of C6H4 layers coated with BF3 groups either side. The fluorinated walls leave enough space to coordinate the potassium cations of which one is slightly pulled towards the ring centre by the water molecule.
The study of non-covalent interactions, and in particular of the contribution of organic fluorine in the formation of different supramolecular motifs, is an expanding area of research amongst the scientific community and has recently gained much interest both in crystal engineering for the systematic design of advanced functional materials14,15 and in asymmetric synthesis.16 Thus, to gain further insights, the interactions within the crystal were investigated in detail by the use of an NCI (non-covalent interaction) analysis,17 which is an informative and illustrative tool to display hydrogen bonds and weak inter- and intramolecular interactions based on the calculated electron density. In addition, we have adopted Bader's atoms in molecules (AIM) concept for identifying a bond path and a bond critical point (BCP) from the electron density.18 In Fig. 4, the water OH⋯π interaction (vide supra) is clearly identified and visualized as an interaction surface. The hydrogen bond critical point is visualized as a light blue sphere and the hydrogen bond path is seen as a dotted line. The hydrogen bond strength was quantified to be ca. −8 kcal mol−1 by DFT calculations.19 It is also found that H2O interacts with the potassium cation K5, quantified to ca. −7 kcal mol−1. In addition, the two aromatic rings are stabilized by side-on dispersive CH⋯π interactions as visualized by the interaction surface and the two BCP spheres and bond paths. Interestingly, the fluorines in the BF3 group are observed to feature three distinctly different interactions (Fig. 4): F⋯F halogen bond interaction,15 CH⋯F interaction to an aromatic hydrogen, and in addition also to the potassium cation. A more detailed characterization of these interactions is found in Fig. S1 in the ESI.† The short distances between K⋯C were, by the BCP and bond path analysis, actually found to be due to agostic interactions20 between potassium and the aromatic CH hydrogens rather than due to the carbons. This conclusion was supported by an NBO-analysis, which showed electron delocalisation from the two aromatic C–H bonds to the potassium cations (for further details, see Fig. S2, ESI†). Thus, by the use of the NCI and BCP analysis we have been able to demonstrate the presence of K⋯F, K⋯O, K⋯HC, OH⋯π, CH⋯π, F⋯F and CH⋯F inter- and intramolecular interactions. It is thus manifested that the fluorines in the trifluoroborate group are of great importance for stabilization and formation of the crystal structure of compound 2.
Fig. 4 Non-covalent interaction (NCI) analysis of extracts of the crystal structure of compound 2. BCP = bond critical point marked with light-blue spheres and bond paths with dotted lines. |
Footnotes |
† Electronic supplementary information (ESI) available: Structural characterization and crystallographic data of compound 2. Computational details and structural analysis. CCDC 1402900. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c5dt02020d |
‡ A. F. and S. O. N. L. contributed equally to this work. |
§ Torsion angles C4–C10–B1–F2 = −88.59°, C4–C10–B1–F5 = 153.67°, C4–C10–B1–F7 = 30.19°, C1–C2–B2–F1 = 86.21°, C1–C2–B2–F8 = −156.72°, C1–C2–B2–F6 = −33.34°, C8–C3–B3–F9 = −89.42°, C8–C3–B3–F4 = 150.34°, and C8–C3–B3–F3 = 32.36°. |
¶ The solution structure of 2 exhibits a single set of signals: 1H-NMR (400 MHz, DMSO-d6): δ = 7.04 (s, 4H); 13C-NMR (150 MHz, DMSO-d6): δ = 145.4 (br s); 19F-NMR (376 MHz, DMSO-d6): δ = −137.5 (br s); 11B-NMR (192 MHz, DMSO-d6): δ = 4.38 (br s). |
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