Benita
Barton
*,
Brandon
Barnardo
and
Eric C.
Hosten
Department of Chemistry, Nelson Mandela University, PO Box 77000, Port Elizabeth, 6031, South Africa. E-mail: benita.barton@mandela.ac.za
First published on 22nd September 2021
In the present investigation, we compare the host and selectivity behaviour of two compounds, namely α,α-diphenyl-9,10-dihydro-9,10-ethanoanthracene-11-methanol H1 and α,α-bis(p-chlorophenyl)-9,10-dihydro-9,10-ethanoanthracene-11-methanol H2, when recrystallized from both singular and mixed isomers comprising the xylenes (o-Xy, m-Xy and p-Xy) and ethylbenzene (EB) as potential guest solvents. H1 formed a complex with o-Xy alone in the single solvent experiments, while H2 included all four of these aromatic compounds. In equimolar guest competition experiments, H1 only crystallized from binary mixtures where o-Xy was present, and high selectivities for this guest were observed in these instances (84.5–93.7%). The other binary mixtures ultimately presented as gels, and H1 therefore failed to crystallize from these. In fact, this was true also for all ternary and quaternary experiments with H1, even when o-Xy was present. H2, on the other hand, consistently formed mixed complexes from all of the solutions employed. However, its selectivity for any particular guest was unremarkable. Guest/guest competition experiments using both equimolar and non-equimolar mixtures revealed that H1 may be employed to purify o-Xy/m-Xy, o-Xy/p-Xy and o-Xy/EB binary mixtures, especially when these solutions comprised 50% or more o-Xy (these experiments all favoured o-Xy). SCXRD analyses were employed to understand the moderate preference of H2 for o-Xy: only this guest was involved in contacts with the host compound, two in number, that measured significantly less than the sum of the van der Waals radii of the atoms involved. Additionally, Hirshfeld surface investigations showed that H2, through its chlorine atoms, was involved in the greater number of contacts with the preferred o-Xy guest compound. Thermal analyses, however, proved less useful in understanding these selectivity data.
In our laboratories, we have spent much time and resources on this very challenge by preparing host compounds derived from tartaric acid, xanthone and thioxanthone, and presenting these with various mixtures of the xylene and ethylbenzene isomers (o-Xy, m-Xy, p-Xy and EB).6–11 Excellent selectivities (95–97%) were observed for p-Xy when the host compounds were N,N′-bis(9-phenyl-9-xanthenyl)ethylenediamine7 and N,N′-bis(9-phenyl-9-thioxanthenyl)ethylenediamine,8 alluding to the possibility of employing these host compounds for successful separations of certain mixtures of these isomers. Several other researchers have also focussed their energies on this industrial problem, and reports by Wicht3 and Nassimbeni et al.12 serve as fitting examples thereof. An exciting article by Day et al.13 investigated both perethylated pillar[5]- and pillar[6]-arenes (EtP5 and EtP6) for this function and found that the latter arene performed extremely well, separating the para- from the meta- and ortho-isomers with 90% specificity. Single crystal diffraction analyses revealed the para-xylene molecule to be located almost exactly in the middle of the cavity of EtP6. There have, furthermore, been numerous reports detailing the employment of metal- and covalent-organic frameworks (MOFs and COFs), as well as zeolites, for the separation of these aromatic C8H10 isomers.14–16
Notwithstanding the myriad reports dealing with the separation of Xy/EB mixtures, the quest for different host compounds with greater advantages relative to known contenders in these guest/guest competition conditions remains ongoing. Host compounds that present fewer complications with respect to their syntheses and yields, that are obtainable readily and at low cost, and that have enhanced selectivities for one or another of these guest components, are constantly being sought. To this end, we have recently embarked upon assessing the roof-shaped host compounds, the brainchild of Prof Edwin Weber,17 for their adeptness as separation or purification tools for Xy/EB mixtures. The roof-shaped host compound trans-9,10-dihydro-9,10-ethanoanthracene-11,12-dicarboxylic acid displayed remarkable selectivity for p-Xy (94–97%) when the other guest present was either o-Xy or m-Xy, even when the concentration of p-Xy in solution was as low as approximately 30%.18 Its dimethyl ester, however, performed poorly in analogous conditions. In a similar fashion, competition experiments employing trans-α,α,α′,α′-tetraphenyl-9,10-dihydro-9,10-ethanoanthracene-11,12-dimethanol and trans-α,α,α′,α′-tetra(p-chlorophenyl)-9,10-dihydro-9,10-ethanoanthracene-11,12-dimethanol showed the latter to be significantly more selective than the former, and the selectivity for m-Xy from o-Xy/m-Xy mixtures exceeded 91%.19 The behaviour of the former unsubstituted phenyl derivative was only ordinary in most of the recrystallization experiments conducted in that work.
In the current investigation, we report on the behaviour of related roof-shaped host compounds α,α-diphenyl-9,10-dihydro-9,10-ethanoanthracene-11-methanol H1 and α,α-bis(p-chlorophenyl)-9,10-dihydro-9,10-ethanoanthracene-11-methanol H2 when these were recrystallized from various mixtures containing Xy/EB (Scheme 1). While Weber et al.17 briefly mentioned that the selectivity of H1 was for o-Xy when presented with binary o-Xy/benzene, o-Xy/toluene, o-Xy/m-Xy and o-Xy/p-Xy solutions, no further guest/guest competitions were carried out with this host compound in that or any other reports from the literature. Similarly, the literature contains no record of similar experiments with H2. Only two reports were uncovered that noted the single solvent inclusion complexes formed by H1 with acetone and toluene,20 and by H2 with cyclohexylamine and ethyl acetate,21 but no further investigations were conducted. We report here on all selectivity data obtained after analyses of solids emanating from the recrystallization experiments of H1 and H2 from these Xy/EB mixtures. Additionally, this report provides information from single crystal diffraction analyses, where five novel crystal structures are elucidated, as well as the results obtained from thermoanalytical experiments on these complexes.
Scheme 1 Structures of roof-shaped host compounds H1 and H2, and the potential xylene and ethylbenzene guest isomers. |
o-Xy | m-Xy | p-Xy | EB | H1 | H2 |
---|---|---|---|---|---|
G:G ratios (% e.s.d.s) | G:G ratios (% e.s.d.s) | ||||
a The data contained herein were obtained from GC-MS analyses and are the averages of two analogous experiments; % e.s.d.s are thus provided in parentheses. b In all cases where complexation was successful, the overall H:G ratio, obtained from 1H-NMR spectroscopy, was consistently 1:1. c Crystallization did not occur, and a gel remained in the vessel. d The results obtained from many different quaternary mixture experiments and H2 afforded mixed complexes in which both the preferred guest species and the extent of selectivity were inconsistent and thus unreliable. | |||||
X | X | 87.3:12.7 (0.7) | 66.8:33.2 (1.2) | ||
X | X | 84.5:15.5 (0.1) | 73.9:26.1 (1.6) | ||
X | X | 93.7:6.3 (0.5) | 74.6:25.4 (1.9) | ||
X | X | 61.7:38.3 (1.4) | |||
X | X | 53.3:46.7 (1.0) | |||
X | X | 71.8:28.2 (1.0) | |||
X | X | X | 38.4:40.1:21.5 (0.9:0.4:1.1) | ||
X | X | X | 1.7:48.4:49.9 (0.2:0.9:0.7) | ||
X | X | X | 54.9:22.8:22.3 (1.0:0.5:1.4) | ||
X | X | X | 50.0:30.6:19.4 (1.3:0.4:1.8) | ||
X | X | X | X |
Remarkably, H1 only crystallized out in binary mixtures that contained o-Xy. The other binary guest combinations afforded only gels (no crystallization was observed in these instances). In fact, all other experiments involving H1 failed to afford any crystals at all, even the ternary and quaternary solutions in which o-Xy was present. Notably, the preference for o-Xy in the successful recrystallizations was significant (84.5–93.7%) and, considering that only o-Xy formed a complex with H1 in the single solvent experiments (Table 1), this selectivity behaviour was somewhat anticipated. However, what was not predicted was the poor crystallinity of this host compound in the absence of o-Xy in the remaining binary guest combinations and in any ternary or higher combinations of these organic solvents, even where o-Xy was present. Ultimately, however, it may be concluded that H1 would serve as a highly efficient host compound for the purification of o-Xy in binary mixtures where the other guest is either m-Xy, p-Xy or EB and, more especially, in the latter case, by employing host–guest chemistry protocols.
In comparison to H1, host compound H2 was only moderate in its selectivity behaviour when recrystallized from these mixed guests. Optimal results were obtained in the binary experiments in which o-Xy was present, with some preference being noted for this guest compound (66.8–74.6%). In the absence of o-Xy, the meta isomer was favoured in m-Xy/p-Xy (61.7%), and p-Xy in p-Xy/EB (71.8%), while the m-Xy/EB experiment afforded crystals only slightly enriched with m-Xy (53.3%). Finally, all of the ternary experiments resulted in mixed complexes where the host selectivity behaviour was poor (40.1–54.9%). Interestingly, the data obtained from a number of different quaternary mixture experiments revealed the host selectivity to be inconsistent in both its preferred guest species and also the extent of its selectivity. These data were thus not provided here. Overall, then, this host compound would thus not be suitable for the efficient purification of any of these combinations of solvents.
The three profiles obtained for H1, o-Xy/m-Xy (Fig. S1a†), o-Xy/p-Xy (Fig. S1b†) and o-Xy/EB (Fig. S1c†), showed that mixed complexes were formed in each instance and that most of these were all considerably enriched with o-Xy (note that none of the other binary experiments afforded crystals, and gels remained behind in the glass vessels). These results are not surprising given that only o-Xy was enclathrated by H1 in the single solvent experiments (Table 1). The averaged K values were determined to be 4.9, 6.0 and 5.0, respectively. From Fig. S1a,† it is feasible to propose H1 as a host candidate for the purification of mixtures of o-Xy and m-Xy where the former is present in quantities close to and greater than 50% while, similarly, o-Xy/p-Xy mixtures (Fig. S1b†) may be purified when the molar ratio of o-Xy is between 60 and 80% of the solution. In all these aforementioned experiments, the crystals that resulted contained almost 90% or more o-Xy. The o-Xy/EB experiment (Fig. S1c†), however, differed somewhat in that only the 50:50 mixture produced crystals with significantly enhanced quantities of o-Xy. The experiment was repeated thrice in order to ensure that this result was not an outlier and, each time, the resultant crystals contained close to 95% o-Xy. In fact, the K value at this point was, satisfyingly, 13.8, indicative that H1 may be employed successfully to separate such mixtures. Otherwise, in the case of this profile, the behaviour of H1 appeared rather unpredictable, especially when the solution contained just over 40% o-Xy. Once more, this experiment was repeated with very little change in the observed result.
In the binary experiments with H2, the host selectivity was much reduced in each case relative to analogous experiments with H1. Only in three of these profiles was it observed that H2 preferred only one guest, namely in the o-Xy/m-Xy (Fig. S2a†), o-Xy/EB (Fig. S2c†) and p-Xy/EB (Fig. S2f†) solutions, where o-Xy, o-Xy and p-Xy were favoured, respectively. Averaged K values were, however, low (1.6–2.4). In the remaining three experiments (Fig. S2b, S2d and S2e†), the behaviour of H2 was dependent on the guest concentrations in the solutions and all calculated K values were unremarkable (1.9–3.2).
To conclude, the preferential behaviour of H1 in the binary solutions was considerably enhanced and always in favour of o-Xy, alluding to the possibility that this host compound may be employed to purify these mixtures. This is especially the case when these solutions contained more of the o-Xy guest species in the case of o-Xy/m-Xy and o-Xy/p-Xy mixtures, or exactly 50% o-Xy in the case of o-Xy/EB. H2, on the other hand, displayed poor selectivity and even ambivalence in certain instances, and would not be a candidate for such purifications.
H1·o-Xy | H2·o-Xy | H2·m-Xy | H2·p-Xy | H2·EB | |
---|---|---|---|---|---|
Chemical formula | C29H24O·C8H10 | C29H22Cl2O·C8H10 | C29H22Cl2O·C8H10 | C29H22Cl2O·C8H10 | C29H22Cl2O·C8H10 |
Formula weight | 494.64 | 563.52 | 563.52 | 563.52 | 563.52 |
Crystal system | Monoclinic | Triclinic | Triclinic | Triclinic | Triclinic |
Space group | P21/c | P | P | P | P |
μ (Mo-Kα)/mm−1 | 0.069 | 0.240 | 0.241 | 0.248 | 0.248 |
a/Å | 9.8100(6) | 9.760(4) | 9.830(3) | 10.3172(19) | 9.8151(4) |
b/Å | 30.3835(16) | 10.850(4) | 10.658(3) | 12.742(2) | 10.9036(5) |
c/Å | 9.5691(6) | 15.146(5) | 15.343(4) | 13.082(2) | 14.5415(6) |
Alpha/° | 90 | 98.370(17) | 96.197(10) | 67.795(9) | 94.486(2) |
Beta/° | 104.685(2) | 96.251(17) | 96.104(11) | 71.424(8) | 97.7538(19) |
Gamma/° | 90 | 103.375(17) | 105.604(11) | 72.877(9) | 104.6528(19) |
V/Å3 | 2759.0(3) | 1526.8(10) | 1523.7(8) | 1479.3(4) | 1481.57(11) |
Z | 4 | 2 | 2 | 2 | 2 |
F(000) | 1056 | 592 | 592 | 592 | 592 |
Temp./K | 200 | 296 | 296 | 296 | 200 |
Restraints | 0 | 124 | 126 | 0 | 0 |
Nref | 6848 | 7515 | 7345 | 7386 | 7364 |
Npar | 347 | 369 | 416 | 364 | 363 |
R | 0.0530 | 0.0527 | 0.0462 | 0.0459 | 0.0429 |
wR2 | 0.1309 | 0.1610 | 0.1544 | 0.1341 | 0.1195 |
S | 1.04 | 1.05 | 1.07 | 1.02 | 1.03 |
θ min–max/° | 2.1, 28.3 | 2.0, 28.5 | 2.0, 28.4 | 1.7, 28.5 | 1.9, 28.3 |
Tot. data | 83453 | 21529 | 59921 | 61561 | 53899 |
Unique data | 6848 | 7515 | 7345 | 7386 | 7364 |
Observed data [I > 2.0 sigma(I)] | 5197 | 4946 | 4675 | 5264 | 5923 |
R int | 0.028 | 0.027 | 0.054 | 0.041 | 0.019 |
Completeness | 1.000 | 0.994 | 0.997 | 0.994 | 1.000 |
Min. resd. dens. (e Å−3) | −0.25 | −0.46 | −0.43 | −0.45 | −0.40 |
Max. resd. dens. (e Å−3) | 0.24 | 0.47 | 0.36 | 0.36 | 0.32 |
Illustrative host⋯guest unit cell and packing diagrams are provided in Fig. 1a–c (left) which were prepared using Mercury software27 (here, the H2·o-Xy illustration represents also H2·m-Xy and H2·EB, the host packing in each being isostructural). Also given here are the void diagrams (right, yellow) which demonstrate the nature of the guest accommodation, and which were obtained by removing the guests from the packing calculations. All guests appeared to occupy constricted channels in the host crystals.
Surprisingly, no classical host⋯host intermolecular H-bonding could be identified in any of these complexes, but two or three non-classical interactions of this type were present in each one, involving either the host protons of the free aromatic ring systems or the roof methylene protons and the oxygen atom of the hydroxyl functionality. These were all intramolecular in nature, maintaining the host molecular geometry, and measured between 2.31 and 2.56 Å (H⋯A) with associated angles between 102 and 106°. Fig. 2a and b are illustrations depicting the two non-classical H-bonding interactions employing H1·o-Xy and H2·o-Xy as representative examples, respectively, where guest molecules have been omitted for clarity.
Furthermore, all complexes of H2 presented intermolecular host⋯host π⋯π and intramolecular host⋯host O–H⋯π interactions that assisted in both packing the host molecules in three dimensions and maintaining their geometry, and these are illustrated in Fig. 3a and b using H2·p-Xy (3.64 Å, with a slippage of 1.02 Å) and H2·EB (H⋯Cg, 2.58 Å, with an associated angle of 156°) as examples, respectively (again, the guest molecules have been removed). Note that these interaction types were not present in H1·o-Xy and, in the latter instance, the bond between the host hydrogen and oxygen atoms was oriented in a significantly less perpendicular fashion relative to the adjacent fused aromatic ring of H1, ensuring the absence of any meaningful intramolecular host⋯host O–H⋯π interactions. This is illustrated in Fig. 3c where the red areas are the calculated planes of the relevant fused aromatic ring and the C–O–H group.
However, an intermolecular O–H⋯π interaction was identified in H1·o-Xy where the hydroxyl group of one host molecule interacts favourably with an aromatic ring double bond on a neighbouring host molecule. This interaction measured 2.75 Å which is significantly less than the sum of the van der Waals radii (2.90 Å).
Any other π⋯π interactions in these complexes were not significant, and guest retention was not reliant upon this interaction type.
Both host and guest species in H1·o-Xy experienced C–H⋯π interactions involving the host free aromatic protons and the guest centroid (2.78 and 2.97 Å, 151 and 136°) (H⋯π, C–H⋯π) as well as the guest aromatic and methyl protons and the host aromatic centres of gravity (2.88 and 2.96 Å, 153 and 150°). These were further accompanied by (host)ArC–H⋯C–C(guest) (2.87 Å, 142°) and (guest)C–H⋯H–C(host) (2.36 Å, 174°) stabilizing contacts. All of the aforementioned interactions were thus responsible for the retention of the o-Xy guest within the H1 crystals.
The host⋯guest interactions that were identified in the four complexes with H2 are summarized in Table 4 for ease of comparison.
Interaction type | H2·o-Xy | H2·m-Xy | H2·p-Xy | H2·EB |
---|---|---|---|---|
a < denotes contacts less than the sum of the van der Waals radii and ≪ contacts less than this sum minus 0.2 Å. | ||||
(Host)C–H⋯π(guest) | 2.86 Å, 139° | 2.94 Å, 142° | 2.74 Å, 154° | 2.91 Å, 152° |
2.83 Å, 150° | 2.78 Å, 150° | |||
2.82 Å, 152° | ||||
(Guest)C–H⋯π(host) | 2.91 Å, 150° | 2.83 Å, 166° | 2.95 Å, 154° | 2.97 Å, 143° |
2.95 Å, 131° | 2.93 Å, 125° | |||
2.54 Å, 157° | 2.92 Å, 140° | |||
(Guest)C–H⋯C–C(host) | 2.77 Å, 151°, < | 2.84 Å, 136°, < | None | None |
2.24 Å, 132°, ≪ | 2.81 Å, 150°, < | |||
2.80 Å, 151°, < | ||||
(Host)C–C⋯H–C(guest) | 2.86 Å, 153°, < | None | None | None |
(Host)C–H⋯H–C(guest) | 1.96 Å, 142°, ≪ | None | None | None |
(Host)C–H⋯C–C(guest) | 2.85 Å, 153°, < | None | None | 2.89 Å, 136°, < |
Both the preferred o-Xy guest as well as m-Xy experienced a large number of stabilizing host/guest⋯guest/host interactions (Table 4) but only o-Xy was involved in contacts that measured significantly less than the sum of the van der Waals radii of the atoms involved. Two such close interactions were observed, namely of the (guest)C–H⋯C–C(host) (2.24 Å, 132°) and (host)C–H⋯H–C(guest) (1.96 Å, 142°) types. These interactions are significant and certainly contribute towards the affinity of H2 for o-Xy. p-Xy and EB, on the other hand, were involved in only very few interactions with this host compound.
In order to further investigate the affinity of H2 for o-Xy, we considered Hirshfeld surface analyses and their associated two-dimensional fingerprint plots. These three-dimensional surfaces are used to describe the immediate surroundings of molecules and to explore, quantitatively, the various host⋯guest and guest⋯host interactions.28 Here, we generated these surfaces around the guest molecules using Crystal Explorer 17 software,29 and these data were then translated into the fingerprint plots. In Fig. 4a–d, de and di are the distances to the nearest atom outside and inside the guest surface, respectively (note that we considered the two disordered guest components in H2·o-Xy and H2·m-Xy separately). In particular, we analysed the interactions of the chlorine atoms of the host compound with the guest species, and these are depicted as the blue highlights in these figures. In all but one case, the host chlorine atoms interacted only with guest hydrogen atoms [the exception is (host)Cl⋯C(guest) interactions in H2·p-Xy, but this contribution was only small (0.2%) compared with the (host)Cl⋯H(guest) interactions (2.1%)].
In order to visually describe these observations, a bar graph was prepared (Fig. 5) and, interestingly, overall, the preferred guest species of H2 (o-Xy) was involved in a greater percentage of stabilizing interactions with the chlorine atoms of the host molecule (6.5, 8.3%) than the other guest molecules. This observation may further explain this host compound's selection of o-Xy. Additionally, and as alluded to before, the host packing in H2·p-Xy was unique compared with the other three complexes (which displayed isostructural host packing), and this is evident in Fig. 5: the percentage of host chlorine atom interactions with p-Xy was significantly lower (2.3%) than in the other complexes (5.0–8.3%), and this may well be as a result of the different packing in this crystal.
Fig. 5 A quantitative depiction of the percentage of host chlorine atom interactions with any guest atoms (more usually hydrogen). |
Complex | T on /°C | Measured mass loss/% | Expected mass loss/% |
---|---|---|---|
a T on is the onset temperature for the guest release process and is determined from the DTG trace. b The complex was unstable at room temperature. | |||
H1·o-Xy | 64.0 | 18.3 | 21.5 |
H2·o-Xy | 108.8 | 16.0 | 18.8 |
H2·m-Xy | 120.0 | 16.8 | 18.8 |
H2·p-Xy | 100.7 | 15.6 | 18.8 |
H2·EB | 18.8 |
Guest removal from H1·o-Xy occurred in two broad steps, initiating at 64.0 °C, with the host melting endotherm peaking at 189.4 °C prior to which all of the guest compound had escaped (Fig. S3a,†Table 5). Prof. Weber reported that pure H1 melted between 191 and 192 °C.17 On the other hand, the lower melting host H2 (124–125 °C (ref. 17)) experienced concomitant guest release and host melt processes. Furthermore, all of the guests of H2, with the exception of EB, were released in a single step (Fig. S3b–e†); the complex containing EB was not stable at room temperature and was released in two steps, the first of these occurring right from the outset of the experiment, and hence accurate Ton and mass loss measurements could not be made in this particular case. Notably, this guest was often discriminated against in the competition experiments (Table 2), and the poor thermal stability of this complex may explain this observation. We also observed that the preference of H2 for o-Xy when mixed with any other guest could not be explained using these thermal data: the most stable complex was that with m-Xy (Ton 120.0 °C), while the complex containing o-Xy appeared less stable (108.8 °C). Also notable is that measured and expected mass losses were in similar to lower-than-expected ranges.
Footnote |
† Electronic supplementary information (ESI) available: Fig. S1a–c (H1) and S2a–f (H2) (ESI) are the selectivity profiles that were obtained after plotting Z (the mole ratio of GA or GB in the host crystals) against X (the mole ratio of the same guest in the solution). Fig. S3a–e are the overlaid DSC, TG and DTG traces for H1·o-Xy, H2·o-Xy, H2·m-Xy, H2·p-Xy and H2·EB, respectively. CCDC numbers 2088997 (H1·o-Xy), 2088998 (H2·o-Xy), 2088999 (H2·m-Xy), 2089000 (H2·p-Xy) and 2089001 (H2·EB). For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/d1ce01149a |
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