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Selectivity behaviour of two roof-shaped host compounds in the presence of xylene and ethylbenzene guest mixtures

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

Received 26th August 2021 , Accepted 21st September 2021

First published on 22nd September 2021


Abstract

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.


1. Introduction

Very recently, there has been much interest in the field of host–guest chemistry as investigations continue in the search for efficient alternative separation or purification protocols for combinations of the xylenes and ethylbenzene.1–3 Due to their narrow boiling range (136.2–144.5 °C) when crude oil is distilled, these isomeric compounds distil across more or less simultaneously and are thus isolated as a mixture. Further tedious, costly and energy-intensive fractional distillations/crystallizations are then warranted in order to obtain each component in pure form and, oftentimes, these processes may not be effective enough to afford these compounds with optimal purities for further synthetic applications.4 As an example, p-xylene is a tremendously important building block towards polyethylene terephthalate (PET), accepted as the most important commercial polyester polymer. The process involves, first, the oxidation of p-xylene to form terephthalic acid which then undergoes an esterification reaction to furnish dimethyl terephthalate (DMT). In order for the polymerization of DMT to PET to be successful, it is required that DMT be extremely pure,5 and this requisite is made all the more difficult to attain if the starting xylene lacked in adequate purity. Hence there exists a need for more efficient, less energy-consuming and lower cost separatory techniques, and host–guest chemistry presents itself as one such alternative protocol. Besides the relatively simple syntheses of the host compounds in most cases, this field of chemistry is a very attractive substitute given the facile recyclability of the host material in such applications, which has a direct consequence on the overall cost of the process and the rampant depletion of fossil fuels.

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.


image file: d1ce01149a-s1.tif
Scheme 1 Structures of roof-shaped host compounds H1 and H2, and the potential xylene and ethylbenzene guest isomers.

2. Experimental

2.1 General

All chemicals and solvents were purchased from Sigma-Aldrich in South Africa and used without further modification. 1H-NMR experiments were conducted on a Bruker Ultrashield Plus 400 MHz spectrometer. GC-MS analyses were carried out using a Young Lin YL6500 gas chromatograph coupled to a flame ionization detector, and dichloromethane was the dissolution solvent for the complexes of both host compounds. For the xylenes and ethylbenzene guest solvents, an Agilent J&W Cyclosil-B column was applicable. The method involved an initial 1 min hold time at 50 °C followed by a ramp of 10 °C min−1 until 90 °C was reached. This temperature was maintained for 3 min during which time the last peak eluted from the column. The flow rate was 1.5 mL min−1 with a split ratio of 1[thin space (1/6-em)]:[thin space (1/6-em)]80. Due to instrument availability, an Agilent 7890A gas chromatograph coupled to an Agilent 5975C VL spectrometer was also used at times; the column remained the same. Again, the method involved an initial hold time of 1 min at 50 °C after which the sample was heated at 0.5 °C min−1 until 52 °C was reached, and then at 0.3 °C min−1 until it reached a temperature of 54 °C. The flow rate was, again, 1.5 mL min−1 and the split ratio 1[thin space (1/6-em)]:[thin space (1/6-em)]100.

2.2 Synthesis of the roof-shaped host compounds H1 and H2

Both roof-shaped host compounds (H1 and H2) were readily synthesized in good yield by considering the methods of Weber et al.17

2.3 Recrystallization experiments of the host compounds from singular solvents

In order to determine whether H1 and H2 are efficient host compounds for o-Xy, m-Xy, p-Xy and EB, each one was recrystallized independently from the four organic solvents. To achieve this, H1 or H2 (0.05 g) was dissolved in an excess of each of these guests (6–7 mmol) in glass vials. The vials were then left open to the ambient conditions which facilitated crystallisation. The crystals were collected under suction and washed with low boiling petroleum ether (40–60 °C). Analysis of these solids was by means of 1H-NMR spectroscopy. The host[thin space (1/6-em)]:[thin space (1/6-em)]guest ratios (H[thin space (1/6-em)]:[thin space (1/6-em)]G) of successfully-formed complexes were calculated by comparing the areas under the peaks for selected host and guest resonance signals.

2.4 Recrystallization experiments of the host compounds from equimolar mixed guests

To investigate the selectivities of H1 and H2 for any of the guest components, each host compound was recrystallized from binary, ternary and quaternary mixtures of these guests where each guest was present in equimolar amounts. Therefore H1 or H2 (approximately 0.05 g) was dissolved in the guest mixture (7 mmol combined amount), and the vials closed and stored in a refrigerator (0 °C). Any crystals that formed in this way were again collected under suction, washed with petroleum ether and analysed by means of GC-MS. These analyses provided the G[thin space (1/6-em)]:[thin space (1/6-em)]G ratios of each of the mixed complexes (as appropriate) while 1H-NMR spectroscopy was employed to determine the overall H[thin space (1/6-em)]:[thin space (1/6-em)]G ratios.

2.5 Recrystallization experiments of the host compounds from binary guest mixtures in varying proportions

The selectivity behaviour of each host compound was also assessed in binary guest mixtures where the concentration of each guest component present was varied. The guest molar ratios thus employed approximated 80[thin space (1/6-em)]:[thin space (1/6-em)]20, 60[thin space (1/6-em)]:[thin space (1/6-em)]40, 50[thin space (1/6-em)]:[thin space (1/6-em)]50, 40[thin space (1/6-em)]:[thin space (1/6-em)]60 and 20[thin space (1/6-em)]:[thin space (1/6-em)]80 for guests A (GA) and B (GB), respectively. Thus, after mixing the solvents in these proportions, each host compound (0.05 g) was dissolved in the resultant solution (the combined guest amount remained 7 mmol), and the vials treated in the same manner as in the equimolar experiments. Both phases were analysed by GC-MS, the solution (X) as well as the crystals emanating from the solution (Z). Therefore, these analyses provided the GA[thin space (1/6-em)]:[thin space (1/6-em)]GB ratios in each of the phases, and a plot of Z for GA (or GB) against X for GA (or GB) afforded selectivity profiles which depict the selectivity behaviour of the host compound in such varying conditions.22 The selectivity coefficient, KGA[thin space (1/6-em)]:[thin space (1/6-em)]GB, obtained using the equation KGA[thin space (1/6-em)]:[thin space (1/6-em)]GB = ZGA/ZGB × XGB/XGA, where XGA + XGB = 1, measures the host selectivity. Fig. S1a–c and S2a–f (ESI) were the result of these plots, wherein have been inserted straight lines to demonstrate the behaviour of an unselective host compound (where K = 1) compared with the experimental data points.

2.6 Single crystal X-ray diffraction (SCXRD) analyses

SCXRD experiments were conducted at 200 or 296 K using a Bruker Kappa Apex II diffractometer with graphite-monochromated Mo Kα radiation (λ = 0.71073 Å). APEXII was used for data collection while SAINT was employed for cell refinement and data reduction.23 SHELXT-2018/224 was utilized to solve the structures, and these were refined by means of least-squares procedures using SHELXL-2018/325 together with SHELXLE26 as a graphical interface. All non-hydrogen atoms were refined anisotropically. Carbon-bound hydrogen atoms were added in idealised geometrical positions in a riding model. The hydrogen atoms of the hydroxyl groups were allowed to rotate with a fixed angle around the C–O bond to best fit the experimental electron density. Data were corrected for absorption effects using the numerical method implemented in SADABS.23o-Xy and m-Xy in crystals of H2 were disordered and required the use of various constraints and restraints. The new crystallographic data for the five complexes produced in this work were deposited at the Cambridge Crystallographic Data Centre (CCDC), with CCDC numbers 2088997 (H1·o-Xy), 2088998 (H2·o-Xy), 2088999 (H2·m-Xy), 2089000 (H2·p-Xy) and 2089001 (H2·EB).

2.7 Thermal analyses

Successfully-formed complexes arising from recrystallization experiments of the host compounds from singular guest solvents were analysed by means of thermoanalytical experiments (these solids were recovered as usual and were not further manipulated). The thermal experiments were performed by means of a TA SDT Q600 Module system while resultant data were analysed using TA Universal Analysis 2000 software. Samples were placed in open platinum pans, and an empty pan functioned as the reference. The purge gas was high purity nitrogen. Samples were heated from approximately 40 to 400 °C, and the heating rate was 10 °C min−1. Dependent on instrument availability, some of these analyses were performed using a Perkin Elmer STA6000 simultaneous thermal analyser and analysed using Perkin Elmer Pyris 13 thermal analysis software. In this instance, an empty ceramic pan was used for both the reference and then the sample run.

3. Results and discussion

3.1 Recrystallization experiments of the host compounds from singular solvents

The 1H-NMR results obtained after isolating and analysing the crystals emanating from the recrystallization experiments of H1 and H2 from each of the xylenes and EB are summarized in Table 1. Interestingly, H1 was significantly more selective in its behaviour compared with H2, enclathrating only o-Xy; in experiments with m-Xy, p-Xy and EB, only apohost host H1 crystallized from the solutions. The p-chloro host derivative H2, on the other hand, formed complexes with each of the four isomers. In all successful complexation experiments, the preferred H[thin space (1/6-em)]:[thin space (1/6-em)]G ratio remained 1[thin space (1/6-em)]:[thin space (1/6-em)]1.
Table 1 H[thin space (1/6-em)]:[thin space (1/6-em)]G ratios of complexes formed upon recrystallization of compounds H1 and H2 from the xylenes and EBa
Guest H1[thin space (1/6-em)]:[thin space (1/6-em)]G ratio H2[thin space (1/6-em)]:[thin space (1/6-em)]G ratio
a The H[thin space (1/6-em)]:[thin space (1/6-em)]G ratios were obtained from 1H-NMR spectra of the resultant crystals from each recrystallization experiment. b The guest was not enclathrated and only apohost crystallized from these solutions.
o-Xy 1[thin space (1/6-em)]:[thin space (1/6-em)]1 1[thin space (1/6-em)]:[thin space (1/6-em)]1
m-Xy 1[thin space (1/6-em)]:[thin space (1/6-em)]1
p-Xy 1[thin space (1/6-em)]:[thin space (1/6-em)]1
EB 1[thin space (1/6-em)]:[thin space (1/6-em)]1


3.2 Recrystallization experiments of the host compounds from equimolar mixed guests

Table 2 summarizes the GC-MS (for G[thin space (1/6-em)]:[thin space (1/6-em)]G ratios) and 1H-NMR (for overall H[thin space (1/6-em)]:[thin space (1/6-em)]G ratios) data obtained upon recrystallizing each of the host compounds from mixtures comprising equimolar amounts of every possible binary, ternary and quaternary combination of the four guest isomers. These experiments were conducted in duplicate, and this table contains the averaged values. Percentage e.s.d.s are, furthermore, provided in parentheses.
Table 2 Mixed complexes formed by H1 and H2 after recrystallization from the various equimolar solutions of the xylenes and EBa,b
o-Xy m-Xy p-Xy EB H1 H2
G[thin space (1/6-em)]:[thin space (1/6-em)]G ratios (% e.s.d.s) G[thin space (1/6-em)]:[thin space (1/6-em)]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[thin space (1/6-em)]:[thin space (1/6-em)]G ratio, obtained from 1H-NMR spectroscopy, was consistently 1[thin space (1/6-em)]:[thin space (1/6-em)]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[thin space (1/6-em)]:[thin space (1/6-em)]12.7 (0.7) 66.8[thin space (1/6-em)]:[thin space (1/6-em)]33.2 (1.2)
X X 84.5[thin space (1/6-em)]:[thin space (1/6-em)]15.5 (0.1) 73.9[thin space (1/6-em)]:[thin space (1/6-em)]26.1 (1.6)
X X 93.7[thin space (1/6-em)]:[thin space (1/6-em)]6.3 (0.5) 74.6[thin space (1/6-em)]:[thin space (1/6-em)]25.4 (1.9)
X X 61.7[thin space (1/6-em)]:[thin space (1/6-em)]38.3 (1.4)
X X 53.3[thin space (1/6-em)]:[thin space (1/6-em)]46.7 (1.0)
X X 71.8[thin space (1/6-em)]:[thin space (1/6-em)]28.2 (1.0)
X X X 38.4[thin space (1/6-em)]:[thin space (1/6-em)]40.1[thin space (1/6-em)]:[thin space (1/6-em)]21.5 (0.9[thin space (1/6-em)]:[thin space (1/6-em)]0.4[thin space (1/6-em)]:[thin space (1/6-em)]1.1)
X X X 1.7[thin space (1/6-em)]:[thin space (1/6-em)]48.4[thin space (1/6-em)]:[thin space (1/6-em)]49.9 (0.2[thin space (1/6-em)]:[thin space (1/6-em)]0.9[thin space (1/6-em)]:[thin space (1/6-em)]0.7)
X X X 54.9[thin space (1/6-em)]:[thin space (1/6-em)]22.8[thin space (1/6-em)]:[thin space (1/6-em)]22.3 (1.0[thin space (1/6-em)]:[thin space (1/6-em)]0.5[thin space (1/6-em)]:[thin space (1/6-em)]1.4)
X X X 50.0[thin space (1/6-em)]:[thin space (1/6-em)]30.6[thin space (1/6-em)]:[thin space (1/6-em)]19.4 (1.3[thin space (1/6-em)]:[thin space (1/6-em)]0.4[thin space (1/6-em)]:[thin space (1/6-em)]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.

3.3 Recrystallization experiments of the host compounds from binary guest mixtures in varying proportions

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).

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[thin space (1/6-em)]:[thin space (1/6-em)]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.

3.4 SCXRD analyses

Table 3 summarizes all the relevant crystallographic data for the five complexes produced in this work. H1·o-Xy crystallized in the monoclinic crystal system and space group P21/c, while all four complexes of H2 were solved in the triclinic crystal system and space group [P with combining macron]1. The host packing in three of these H2 inclusion compounds was isostructural, namely in H2·o-Xy, H2·m-Xy and H2·EB, while this packing was unique in H2·p-Xy. Only two guest components displayed disorder in these crystals: o-Xy in H2 required a number of constraints and restraints in order to model it, and m-Xy, also in H2, experienced disorder over two positions.
Table 3 Relevant crystallographic data for the complexes of H1 and H2 with the xylenes and ethylbenzene
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[1 with combining macron] P[1 with combining macron] P[1 with combining macron] P[1 with combining macron]
μ (Mo-Kα)/mm−1 0.069 0.240 0.241 0.248 0.248
a 9.8100(6) 9.760(4) 9.830(3) 10.3172(19) 9.8151(4)
b 30.3835(16) 10.850(4) 10.658(3) 12.742(2) 10.9036(5)
c 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)
V3 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 83[thin space (1/6-em)]453 21[thin space (1/6-em)]529 59[thin space (1/6-em)]921 61[thin space (1/6-em)]561 53[thin space (1/6-em)]899
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.


image file: d1ce01149a-f1.tif
Fig. 1 Unit cell and host–guest packing diagrams (left) and voids (right, yellow) in a) H1·o-Xy, along [100], b) H2·o-Xy (also representing H2·m-Xy and H2·EB), along [010], and c) H2·p-Xy, along [001].

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.


image file: d1ce01149a-f2.tif
Fig. 2 Intramolecular host⋯host non-classical hydrogen bonding interactions maintaining the host molecular geometry of the a) free Ar–H⋯O (in H1·o-Xy) and b) roof HC–H⋯O (in H2·o-Xy) type; guest molecules have been removed 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.


image file: d1ce01149a-f3.tif
Fig. 3 Host⋯host a) intermolecular π⋯π (in H2·p-Xy) and b) intramolecular OH⋯π (in H2·EB) interactions; c) the calculated planes (red) of the adjacent fused aromatic ring system and the C–O–H group of H1 in H1·o-Xy; guest molecules are not shown here.

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.

Table 4 Host⋯guest interactions present in the complexes with H2a
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%)].


image file: d1ce01149a-f4.tif
Fig. 4 Fingerprint plots showing host chlorine atom interactions with a) guest hydrogen atoms in H2·o-Xy (one disordered component, left, and the other, right), b) guest hydrogen atoms in H2·m-Xy (one disordered component, left, and the other, right), c) guest carbon atoms (0.2%, left) and guest hydrogen atoms (2.1%, right) in H2·p-Xy, and d) guest hydrogen atoms in H2·EB.

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.


image file: d1ce01149a-f5.tif
Fig. 5 A quantitative depiction of the percentage of host chlorine atom interactions with any guest atoms (more usually hydrogen).

3.5 Thermal analysis

The thermal data, in the form of overlaid differential scanning calorimetric (DSC), thermogravimetric (TG), and its derivative (DTG), traces obtained after heating each sample at a rate of 10 °C min−1 from approximately 40 to 400 °C, are provided in Fig. S3a–e in the ESI. The onset temperatures for the guest release process (Ton), estimated from the DTG traces, is a measure of the relative thermal stability of each complex, and these data are summarized in Table 5 together with measured and expected mass losses upon complete guest removal from the host crystals.
Table 5 T on measurements and measured and expected mass losses for the complexes of H1 and H2
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.

4. Conclusion

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 were recrystallized from each of the xylenes (o-Xy, m-Xy and p-Xy) and ethylbenzene (EB) to assess their host selectivity towards these solvents. H1 only formed a complex with o-Xy in these conditions while H2 enclathrated each one. Mixed guest solvent competition experiments showed that H1 possessed an enhanced selectivity for o-Xy when the other guest was m-Xy, p-Xy or EB (84.5–93.7%), while no crystals could be recovered from the remaining binary, ternary and quaternary guest combinations. The selectivity of H2 in such competition experiments, on the other hand, was, however, only extremely ordinary (40.1–74.6 °C). This work has demonstrated that H1 may be employed to purify o-Xy/m-Xy, o-Xy/p-Xy and o-Xy/EB binary mixtures when these guests are present in specified concentrations. H2 does not have the ability to serve in this manner. SCXRD analyses showed that the preferred guest of H2, o-Xy, was the only one to experience very short contacts with the host molecule, thus explaining the preference of H2 for this guest. Additionally, data from Hirshfeld surface analyses concurred, and o-Xy experienced a greater percentage of stabilizing interactions with the chlorine atoms of the host compound. However, thermal analyses were less useful in explaining the selectivity order of H2 for these aromatic guest solvents.

Author contributions

Benita Barton: conceptualization; funding acquisition; methodology; project administration; resources; supervision; visualization; writing – original draft. Brandon Barnardo: investigation; methodology; validation. Eric C. Hosten: data curation; formal analysis.

Conflicts of interest

There are no conflicts of interest to declare.

Acknowledgements

Financial support is acknowledged from the Nelson Mandela University and the National Research Foundation (NRF) of South Africa.

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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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