Shofiur
Rahman
a,
Ahmed
Zein
a,
Louise N.
Dawe
b,
Grigory
Shamov
c,
Pall
Thordarson
d and
Paris E.
Georghiou
*a
aDepartment of Chemistry, Memorial University of Newfoundland, St. John's, Newfoundland and Labrador, Canada A1B3X7. E-mail: parisg@mun.ca
bDepartment of Chemistry and Biochemistry, Wilfrid Laurier University, Waterloo, Ontario, Canada N2L 3C5
cWestgrid/ComputeCanada, University of Manitoba, Winnipeg, Manitoba, Canada R3T 2N2
dSchool of Chemistry and the ARC Centre for Excellence in Convergent Bio-Nano Science and Technology, University of New South Wales, Sydney 2052, Australia
First published on 16th June 2015
Calix[4]azulene 1 is shown to be an effective molecular receptor for tetraalkylammonium halide and BF4− salts. The respective binding constants were determined using global-fit analyses of the spectral data from UV-vis absorption titration studies. A DFT study of the putative complexes formed with 1, and the X-ray structure of 1 itself is also reported.
Due to the resemblance of 1 to calix[4]arenes2 the potential for molecular recognition studies with these compounds is an obvious one and due to our own on-going interest in the supramolecular complexation properties of such deep-cavity containing molecular receptors.3a–d We report here our findings with respect to a supramolecular host–guest complexation study of 1 with, in particular, tetraalkylammonium halides and tetrafluoroborate salts. A global analytical fitting4a,b was used to determine the binding or association constants from UV-vis titration experiments. During the course of our investigations, crystals of calix[4]azulene from benzene solution were obtained which permitted an X-ray structural determination.5 Concurrently, a DFT (Density Functional Theory)6 computational study was also conducted on both 1 and its complexes.
The ambient temperature 1H NMR spectrum of 1 shows that the methylene bridge protons appear as a sharp singlet at δ = 4.74 ppm, indicating its conformational flexibility. However, in principle, 1 could potentially adopt cone, partial cone, 1,3- or 1,2-alternate conformations which are analogous to those that are typically associated with calix[4]arenes.2 The relatively low solubility of 1 in the usual NMR solvents however, prevented the determination of a coalescence temperature or energy using low-temperature VT-1H NMR spectroscopy.
Since 1 is a hydrocarbon molecule, we hypothesized that its macrocyclic cavity could serve as a site for molecular recognition with, in particular, aromatic hydrocarbon guest molecules, including e.g. naphthalene, hexamethylbenzene and C60 and C70. However using 1H NMR titration7 experiments no meaningful chemical shift changes for either the guest molecules or 1 were observed. Hence no evidence could be observed for any supramolecular complexation of these types of guests with 1.
Nevertheless, a mole ratio plot from a 1H-NMR titration experiment with tetramethylammonium chloride (TMACl) in CDCl3 as a guest, did reveal that a 1:1 complex of TMACl with 1 formed. The low solubilities however, of both host and guest, precluded accurate determinations of the binding or association constant (Kassoc) in subsequent titration experiments. UV-vis spectroscopic titration experiments nevertheless proved more suitable for the studies with TMACl and the other tetraalkylammonium salts reported herein. It should be noted that although fluorescence spectroscopy is more sensitive than UV-vis spectroscopy, and could therefore be used with more dilute (∼10−5 to 10−3 M) solutions than those needed for either 1H-NMR or UV-vis titrations, fluorescence titration experiments could not be used with calix[4]azulene.8–10
To evaluate the potential effects of other larger tetraalkylammonium groups, the effects of higher homologues of TMAX, namely those of the corresponding tetraethyl and tetra-n-butylammonium salts were examined where possible. Solubility problems encountered with these higher tetraalkylammonium halide homologues, were averted by comparing TMABF4 with tetraethylammonium tetrafluoroborate (TEABF4), and tetra-n-butylammonium tetrafluoroborate (TBABF4) since these salts had higher solubilities in the 9:1 (v/v) CHCl3:CH3OH mixed solvent which was the solvent used for all of the UV-vis titrations. The resulting Kassoc values are shown in Table 1, entries 4–6. The trend observed, namely TMABF4 > TEABF4 > TBABF4 is consistent with the DFT calculations shown in Table 3.
Entry | K assoc (M−1) | |
---|---|---|
Average ± ASFU | ||
1 | TMACl | 7400 ± 0.44% |
2 | TMABr | 3820 ± 1.3% |
3 | TMAI | 2840 ± 1.2% |
4 | TMABF4 | 5920 ± 1.2% |
5 | TEABF4 | 5060 ± 1.5% |
6 | TBABF4 | 3620 ± 1.3% |
For the work reported herein, Chai and Head-Gordon's ωB97xD15 functional, which combines the long-range functional ωB97x with the empirical dispersion correction specially parametrized against each other, was used. B3LYP results are provided for comparison purposes only. The popular B3LYP density functional16 which has often been employed by organic chemists has been shown by many authors, including those cited in ref. 17–20, to have numerous shortcomings. These shortcomings are related to the lack of dispersion interactions and the deficiencies of DFT with self-interaction errors and long-range behavior. In the last decade, in order to amend the poor performance of standard DFT, the following methods were proposed, and have become widely used: the empirical dispersion corrections by Grimme,17,21,22 and the long-range hybrid density functionals of Tsuneda and Hirao20 that, when combined, deliver much improved performance for thermodynamics and structure optimization. The effect is most pronounced for host-guest complexes such as were studied in our work where the interactions are dominated by non-bonded terms.22
The standard 6-31G(d) basis set23 was used for all the atoms. This basis set is small by modern standards but we chose to use it due to the relatively large size of our systems. It was shown that larger basis sets including diffuse functions cause basis set overcompleteness problems for condensed hydrocarbons. In agreement with Fry24 we found that the 6-31G(d) basis set was not reliable for the energies of complexes containing bromide anion; for iodide, non-relativistic all-electron calculations are not accurate. Therefore, for guests and complexes containing atoms other than first row elements (i.e. for TMACl, TMABr, TMAI) we used relativistic ECPs by Hay and Wadt (LANL) along with corresponding LANL2DZ basis set augmented with additional d-, p-polarizational functions.25,26a–c Cartesian Gaussian functions (6D, 7F) were used for the halides' LANL2DZ basis set, to make it consistent with the default setting for the 6-31G(d) basis set. For each of the individual components i.e. tetraalkylammonium salt, calix[4]azulene and the respective corresponding 1:1 supramolecular complexes, unconstrained geometry optimizations were first conducted in the gas phase. Then, geometries were optimized within the continuum solvation model (PCM)27a,b of the chloroform solvent, using default solvent parameters as provided with Gaussian-09 rev D.01. The results are summarized in Tables 2 and 3.
B3LYP/6-31G(d) | kJ mol−1 | B3LYP/6-31G(d) | kJ mol−1 |
---|---|---|---|
Gas phase | CHCl 3 | ||
C i | 0 | C i | 0 |
C 2v Chair | +0.34 | C 2v-1,3-alternate | +0.73 |
C 2v-1,3-alternate | +0.68 | C 2v chair | +0.33 |
ωB97xD/6-31G(d) | kJ mol−1 | ωB97xD/6-31G(d) | kJ mol−1 |
---|---|---|---|
Gas phase | CHCl 3 | ||
C s | 0 | C s | 0 |
C 2v-1,3-alternate | +0.58 | C *s | 0 |
C i | +10.1 | C i | +8.94 |
Inclusion of chloroform solvation does not affect the relative energies of the conformers it can be seen that for B3LYP/6-31G(d) the energy difference between the three studied conformers is negligible, while ωB97xD/6-31G(d) has a marked preference for the Cs-symmetrical “flattened” 1,3-alternate conformer, which can be understood by favourable intra-molecular dispersion interaction between the parallel azulene rings in the isolated molecule. These interactions are absent in B3LYP but are included in the ωB97xD functional. The experimentally observed structure shown in Fig. 2a is probably a result of crystal packing forces. In Table 2, the most stable of the conformers for each of the density functionals were used to compute the “binding” energies of the complexes shown. In one case (shown in Table 2 by the entry marked as C*s) where the ωB97xD/6-31G(d) geometry-optimized C2v-1,3-alternate conformer from the gas phase was subjected to the ωB97xD/6-31G(d) geometry-optimization with the chloroform PCM the resulting conformer had the same Cs-symmetry.
Fig. 4 Geometry-optimized (ωB97xD/6-31G(d)) structures computed for: (a) left: TMACl ⊂ 1; (b) middle: TMABr ⊂ 1; (c) right: TMAI ⊂ 1. |
The “binding” or “interaction” (negative) energies (“BE”) generally decreased in magnitude (i.e. less energetically favoured) in going from the ωB97xD/6-31G(d) gas-phase to the CHCl3-corrected computed values, to the corresponding B3LYP/6-31G(d)-computed values, as summarized in Table 3. On the other hand, the binding constants observed for the tetramethyl-ammonium halides showed the trend: Cl− > Br− > I−. The BE of the complexes were calculated according to eqn (1) where Ecalixazulene is the geometry-optimized energy of calix[4]-azulene 1 and Etetraalkylammonium salt is that of the respective tetraalkylammonium salt. Ecomplex is the geometry-optimized energy of the complex formed from 1 with the respective tetraakylammonium salts.
BE = Ecomplex − Σ(Ecalixazulene + Etetraalkylammonium salt) | (1) |
ωB97xD/6-31G(d) | B3LYP/6-31G(d) | |||
---|---|---|---|---|
Gas phase (kJ mol−1) | CH3Cl (kJ mol−1) | Gas phase (kJ mol−1) | CH3Cl (kJ mol−1) | |
a Note: the values in parentheses are the BEs of the TMAI complexes computed as the corresponding 1,3-alternate conformer of 1. | ||||
TMACl | −113.9 | −77.3 | −33.2 | −13.1 |
TMABr | −118.3 | −80.8 | −34.4 | −14.4 |
TMAI | −133.5 (−121.2)a | −93.0 (−84.0)a | −35.4 | −13.9 |
TMABF4 | −144.6 | −116.9 | −49.9 | −20.8 |
TEABF4 | −129.0 | −111.9 | −29.7 | −8.3 |
TBABF4 | −113.5 | −115.1 | −25.6 | −10.1 |
For the halides and BF4−, inclusion of the solvation effects does not change the trends but decreases the BEs uniformly; this is as it should be due to the relative stabilization of the isolated guest which is more polar. The B3LYP density functional predicts significantly weaker binding energies for missing dispersion interactions. Moreover, it does not reveal much difference in binding between the three TMA halide complexes. The more reliable ωB97xD functional predicts increases in the complexes' stability in the order of Cl− < Br− < I− which is in agreement with our experimental findings. As can be seen in Fig. 4c (for TMAI) and Fig. 5a–c, in order to accommodate both the larger iodide and tetrafluoroborate anion and the larger tetraalkylammonium groups, the conformations of the complexes are no longer 1,3-alternate. For the TMAI, TMABF4 and TEABF4 complexes, partial-cone (“paco”) conformers are adopted and for the TBABF4 complex, a near boat-like Cs-symmetrical conformer, as shown in Fig. 3b for the calix[4]azulene host, is formed. The binding energy trends for the tetrafluoroborate salts TMABF4 > TEABF4 > TBABF4 did parallel the trend seen with the corresponding binding constants which were observed (Table 1). To possibly account for the trends in the BEs of the 1:1 complex formation in these salts, there is presumably a greater degree of entropic loss incurred in forming the complexes as the free rotations within the larger alkyl group chains become restricted within the complex.
Footnote |
† Electronic supplementary information (ESI) available: UV-vis titration; X-ray cif and checkcif files for 1 and .mol coordinates from DFT computations. CCDC [1049866]. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c5ra07802d |
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