Open Access Article
Benita Barton
*,
Muhammad-Ameen Adam and
Eric C. Hosten
Department of Chemistry, Nelson Mandela University, PO Box 77000, Gqeberha (Port Elizabeth), 6031, South Africa. E-mail: benita.barton@mandela.ac.za
First published on 14th April 2026
The crystallization of N,N′-bis(9-(4-methoxyphenyl)-9H-xanthen-9-yl)ethane-1,2-diamine (H) from each of the xylene and ethylbenzene isomers (o-Xy, m-Xy, p-Xy and EB) revealed that only the xylenes formed inclusion compounds with this host species, while EB was not included. The host
:
guest (H
:
G) ratios of the successfully formed complexes were 1
:
1, 1
:
1 and 1
:
2 for the o-Xy, m-Xy and p-Xy complexes, respectively. Guest solvents were also permitted to compete and crystallizations of H from such solutions revealed an unequivocal host selectivity in the order o-Xy > EB > m-Xy > p-Xy. Further binary guest competition experiments also demonstrated that this host species may serve as a purification tool, through host–guest chemistry protocols, of EB and m-Xy solvents that are tainted with small quantities of o-Xy and EB, correspondingly. Single crystal X-ray diffraction (SCXRD) analyses of the three single solvent complexes were employed in order to understand the host selectivity behaviour. The guest molecules in H·o-Xy and H·m-Xy (with guest solvents more preferred by H in the guest competition experiments) were accommodated in endless and unidirectional channels, and all of these guest species experienced (guest)C–H⋯π(host) stabilizing interactions with H. This was not the case for the guest species in H·2(p-Xy) (with the least favoured guest solvent). Here, two distinct types of guest molecules were observed, one being ordered and the other displaying positional disorder over two positions. Both of the latter disorder guest components were involved in this kind of interaction ((guest)C–H⋯π(host)) with H, while the ordered guest species appeared to be held in the complex through, predominantly, steric effects alone, and no (guest)C–H⋯π(host) or other close contacts were identified in this instance. This observation explained the distinct lack of selectivity of H for p-Xy relative to the remaining isomers in the guest competition experiments. Interestingly, the ordered and disordered guest molecules in this complex also occupied separate channel voids in the inclusion compound which were aligned along different axes in the unit cell. Finally, thermal analyses demonstrated that the three single solvent complexes in this investigation possessed comparable relative thermal stabilities as their guest release onset temperatures spanned a narrow range (Ton 39.2–41.7 °C).
Owing to the importance of having processes that achieve these separations effectively that do not rely on the boiling points of these compounds, a number of different strategies have been investigated and demonstrated some promise. These include extractive distillations, chromatography, inorganic membranes, zeolites, polymers, and metal–organic and hydrogen-bonded organic frameworks, to mention only a few.18–24 However, despite the success of some of these separation protocols, many are not attractive, more especially with respect to scalability, recyclability and inflated costs.
Host–guest chemistry is an alternative separatory candidate that may be considered in order to effectively separate Xy/EB mixtures. This field of science relies on the selectivity of the “host compound” for one particular “guest species” when presented with a mixture of guest solvents.25,26 In our own laboratories, this avenue for such separations has been extensively investigated with the view to discovering new host compounds with improved or different selectivities compared with those that are better known. The preferential behaviour of the host compound is dependent upon a number of factors, including the existence of noncovalent interactions in these complexes between the host and guest (e.g., π⋯π stacking, X–H⋯π close contacts, hydrogen bonding (classical and nonclassical) and van der Waals forces), steric influences as well as guest attributes (geometry, functional groups, etc.). To this end, host compounds derived from xanthone, thioxanthone, dibenzosuberone, dibenzosuberenone, tartaric acid and anthracene were designed, synthesized and investigated for their separation potential for mixtures of Xy/EB.27–35 These host species more usually preferred p-Xy and/or o-Xy, while EB and/or the meta isomer remained largely disfavoured.
In the present work, an alternate host compound, N,N′-bis(9-(4-methoxyphenyl)-9H-xanthen-9-yl)ethane-1,2-diamine (H), was assessed for its host potential for each of the Xy/EB isomers through crystallization experiments (Fig. 1). If host ability existed, H was then crystallized from various Xy/EB solutions in order to identify its preferential behaviour under these experimental conditions and to ascertain whether H may serve as a separatory or purification candidate for any of these mixtures. Additionally, all single solvent complexes were subjected to both SCXRD and thermal analyses to elucidate the mode of guest entrapment within the crystals of the complex as well as to determine the relative thermal stabilities of these complexes. The present host compound has not been employed in this manner to date, and we report on the results so-obtained herein.
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| Fig. 1 Structures of N,N′-bis(9-(4-methoxyphenyl)-9H-xanthen-9-yl)ethane-1,2-diamine (H), and the potential guest solvents o-xylene, m-xylene, p-xylene and ethylbenzene (o-Xy, m-Xy, p-Xy and EB). | ||
All 1H-NMR experiments were conducted by means of a Bruker Ultrashield Plus 400 MHz spectrometer with CDCl3 as the deuterated solvent. Topspin 4.4.1 software was employed for spectral data analysis.
The SCXRD experiments for the crystal structures of guest-free H, H·o-Xy, H·m-Xy and H·2(p-Xy) were performed at 200(2) K using a Bruker D8 Quest diffractometer with a Photon II CPAD detector and IμS 3.0 Mo source (Kα, λ = 0.71073 Å). APEX436 was used for data collection and SAINT36 for cell refinement and data reduction. Data were corrected for absorption effects using the multi-scan method implemented in SADABS.37 The structure was solved using SHELXT-2018/238 using a dual-space algorithm and refined by least-squares procedures using SHELXL-2025/139 with SHELXLE40 as a graphical interface. Diagrams were drawn with ORTEP-3 for Windows version 2023.1 (SI).41 All non-hydrogen atoms were refined anisotropically. Carbon-bound H atoms were placed in calculated positions (C–H bond lengths of 0.95 Å for aromatic carbon atoms, 1.00 Å for methine, 0.99 Å for methylene) and were included in the refinement in the riding model approximation, with Uiso(H) set to 1.2Ueq(C). When possible the H atoms of the methyl groups were allowed to rotate with a fixed angle around the C–C bond to best fit the experimental electron density (HFIX 137 in the SHELXL program39) with Uiso(H) set to 1.5Ueq(C) and C–H bond lengths of 0.98 Å; otherwise they were placed in calculated positions.
The nitrogen-bound hydrogens were located on a difference map and, when possible, allowed to refine freely. The crystal structures of guest-free H, H·o-Xy, H·m-Xy and H·2(p-Xy) were deposited at the Cambridge Crystallographic Data Centre and their respective CCDC numbers are 2530251–2530254.
GC-MS analyses were carried out using an Agilent 7890A GC equipped with an Agilent J&W Cyclosil-B column coupled to a flame ionization detector. The method involved an initial 1 min hold time at 50 °C. A ramp rate of 10 °C min−1 was then implemented until a final temperature of 90 °C was reached, and this temperature was maintained for 3 min. The flow rate was 1.5 mL min−1 and the split ratio 1
:
40.
A Perkin Elmer STA 600 module system was employed for the thermal experiments; here, data were analysed by means of Pyris software. Samples were placed in ceramic pans with nitrogen serving as the purge gas. The heating rate was 10 °C min−1 and the temperature range employed was from approximately 40 to 350 °C.
:
guest (H
:
G) ratios by comparing the integrals of applicable host and guest resonance signals.
:
80, 40
:
60, 60
:
40 and 80
:
20 GA
:
GB). These crystallizations were carried out in an identical fashion to the aforementioned equimolar guest experiments. Analyses of the crystals were by means of GC, which provided the guest amounts in the so formed mixed guest complexes. Selectivity profiles were then constructed by plotting ZA (or ZB), the amount of GA (or GB) in the crystals, against XA (or XB), the amount of GA (or GB) in the original solution, according to the equation of Pivovar and colleagues, K = ZA/ZB × XB/XA, where XA + XB = 1.43 These plots provide a visual representation of the host selectivity behaviour in such varying guest proportions. K is the selectivity coefficient and may be calculated for each data point in these plots and serves as a measurement of the host selectivity. It has been reported that K values are required to be 10 or greater for effective separations of binary mixtures in a practical setting.44 When K = 1, the host compound is not selective; this theoretical scenario is represented by the straight diagonal lines that have been inserted into each of these profiles for comparison.
:
G ratios of the three complexes that formed successfully were 1
:
1 (o-Xy and m-Xy) and 1
:
2 (p-Xy) (the applicable 1H-NMR spectra for these complexes are provided in the SI).
:
G ratios of complexes of H when crystallized from each of the xylenes and EB
| o-Xy | m-Xy | p-Xy | EB | Guest ratio | % e.s.d.s |
|---|---|---|---|---|---|
| X | X | 59.9 : 40.1 |
1.4 | ||
| X | X | 86.7 : 13.3 |
0.3 | ||
| X | X | 80.7 : 19.3 |
0.8 | ||
| X | X | 53.5 : 46.5 |
0.7 | ||
| X | X | 45.9 : 54.1 |
2.5 | ||
| X | X | 41.2 : 58.8 |
0.3 | ||
| X | X | X | 53.8 : 34.5 : 11.7 |
0.5 : 0.2 : 0.3 |
|
| X | X | X | 48.1 : 9.6 : 42.3 |
1.9 : 0.3 : 1.56 |
|
| X | X | X | 66.6 : 12.8 : 20.6 |
2.5 : 2.3 : 0.2 |
|
| X | X | X | 9.2 : 9.5 : 81.3 |
0.6 : 0.3 : 0.9 |
|
| X | X | X | X | 36.2 : 19.8 : 8.2 : 35.8 |
1.2 : 1.4 : 0.2 : 2.4 |
A rapid scrutiny of the data contained in Table 2 suggests that H preferred o-Xy whenever it was present, followed by EB and then the meta isomer. Interestingly, p-Xy remained disfavoured in each instance. In more depth, the binary solutions involving o-Xy (o-Xy/m-Xy, o-Xy/p-Xy and o-Xy/EB) afforded crystals enriched in o-Xy, and between 59.9 and 86.7% of this isomer were measured in these mixed complexes. In the absence of o-Xy but the presence of EB in these binary experiments (m-Xy/EB and p-Xy/EB), H selected more of EB (54.1 and 58.8%), while when both o-Xy and EB were not involved (m-Xy/p-Xy), the crystals contained an elevated quantity of the meta isomer (53.5%). These trends continued in the ternary experiments, and o-Xy remained favoured in the o-Xy/m-Xy/p-Xy, o-Xy/m-Xy/EB and o-Xy/p-Xy/EB solutions (53.8, 48.1 and 66.6%, respectively), while in the absence of o-Xy (m-Xy/p-Xy/EB), more of EB (81.3%) was selected. Furthermore, and unsurprisingly, the quaternary solution also revealed an enhanced preference for o-Xy (36.2%). In summary, the host selectivity in these guest mixtures may thus be presented as in the order o-Xy > EB > m-Xy > p-Xy. These results are interesting given that, as mentioned earlier, many of the host compounds prepared in our laboratories more usually preferred p-Xy and/or o-Xy, while EB and/or the meta isomer were mostly disfavoured, and this is certainly not the case in the present investigation, with p-Xy being consistently the least favoured guest species.27–35
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| Fig. 2 Selectivity profiles for the binary guest competition experiments involving a) o-Xy/m-Xy, b) o-Xy/p-Xy, c) o-Xy/EB, d) m-Xy/p-Xy, e) EB/m-Xy and f) EB/p-Xy. | ||
| K values | ||||||
|---|---|---|---|---|---|---|
| Binary mixture | 20 : 80 |
40 : 60 |
50 : 50a |
50 : 50a |
60 : 40 |
80 : 20 |
a In all cases, the 50 : 50 experiments were conducted in duplicate (see section 3.2). |
||||||
| o-Xy/m-Xy | 1.8 (o-Xy) | 1.3 (o-Xy) | 1.4 (o-Xy) | 1.6 (o-Xy) | 1.9 (o-Xy) | 2.4 (o-Xy) |
| o-Xy/p-Xy | 8.8 (p-Xy) | 1.8 (o-Xy) | 6.4 (o-Xy) | 6.7 (o-Xy) | 5.5 (o-Xy) | 6.3 (o-Xy) |
| o-Xy/EB | ∞ (EB) | 1.5 (o-Xy) | 4.3 (o-Xy) | 4.0 (o-Xy) | 5.5 (o-Xy) | 5.2 (o-Xy) |
| m-Xy/p-Xy | 4.5 (p-Xy) | 1.4 (m-Xy) | 1.1 (m-Xy) | 1.2 (m-Xy) | 1.4 (m-Xy) | 4.9 (m-Xy) |
| EB/m-Xy | ∞ (m-Xy) | 1.5 (EB) | 1.3 (EB) | 1.1 (EB) | 1.3 (EB) | 1.6 (EB) |
| EB/p-Xy | 1.2 (EB) | 1.5 (EB) | 1.4 (EB) | 1.4 (EB) | 1.5 (EB) | 1.8 (EB) |
Fig. 2a and f demonstrate that in the o-Xy/m-Xy and EB/p-Xy binary solutions, H was selective for only one guest across the concentration range, namely o-Xy and EB, respectively. On the other hand, Fig. 2b–e reveal that the preferential behaviour of H was guest concentration dependent. In each of these instances, the host compound in the 20/80 mixtures selected more of the guest present in the higher concentration. Therefore, the complexes emanating from the 20/80 o-Xy/p-Xy, o-Xy/EB, m-Xy/p-Xy and EB/m-Xy solutions were enriched in p-Xy, EB, p-Xy and m-Xy, correspondingly. All of the remaining data points in these four plots, however, showed a consistent host preference for the alternative guest solvent, those listed first in these guest pairs.
From Table 3, K was too low (1.1–8.8) in most instances to suggest that H would be an ideal host candidate for these separations through host–guest chemistry. Strikingly, though, two selectivity coefficients were calculated to be infinite as a result of the fact that only one guest species was observed in the so formed complexes. The applicable inclusion compounds were those obtained from the 20/80 o-Xy/EB and 20/80 EB/m-Xy solutions in which only EB and m-Xy, respectively, were detected in the crystals. These results indicate that H may behave as a purification tool for solvents EB and m-Xy that are tainted with, in turn, small quantities of o-Xy and EB.
, while both H·o-Xy and H·m-Xy crystallized in the monoclinic crystal system and, in both cases, the space group was P21/n. In fact, upon a closer inspection of the unit cell parameters of these two complexes, it was clear that the host packing in each one was isostructural.
| H | H·o-Xy | H·m-Xy | H·2(p-Xy) | |
|---|---|---|---|---|
| Chemical formula | C42H36N2O4 | C42H36N2O4, C8H10 | C42H36N2O4, C8H10 | C42H36N2O4, 2(C8H10) |
| Formula weight | 632.73 | 738.89 | 738.89 | 845.04 |
| Crystal system | Triclinic | Monoclinic | Monoclinic | Triclinic |
| Space group | P![]() |
P21/n | P21/n | P![]() |
| μ (Mo-Kα)/mm−1 | 0.084 | 0.078 | 0.080 | 0.075 |
| a/Å | 11.8593(4) | 17.8696(12) | 18.206(3) | 8.6383(3) |
| b/Å | 15.2353(6) | 10.5775(7) | 10.4572(14) | 9.2258(3) |
| c/Å | 16.0329(6) | 22.5364(14) | 21.564(3) | 15.8317(5) |
| Alpha/° | 64.5256(12) | 90 | 90 | 104.060(1) |
| Beta/° | 81.2254(12) | 111.015(2) | 109.528(5) | 91.052(1) |
| Gamma/° | 67.5368(12) | 90 | 90 | 108.317(1) |
| V/Å3 | 2416.52(16) | 3976.4(5) | 3869.3(10) | 1155.74(7) |
| Z | 3 | 4 | 4 | 1 |
| F(000) | 1002 | 1568 | 1568 | 450 |
| Temp./K | 200 | 200 | 200 | 200 |
| Restraints | 0 | 222 | 0 | 60 |
| Nref | 9820 | 8078 | 5663 | 5731 |
| Npar | 665 | 557 | 426 | 335 |
| R | 0.0533 | 0.0760 | 0.1031 | 0.0545 |
| wR2 | 0.1163 | 0.1356 | 0.1802 | 0.1252 |
| S | 1.13 | 1.21 | 1.11 | 1.11 |
| θ min–max/° | 2.0, 26.4 | 2.2, 26.5 | 2.2, 23.5 | 2.4, 28.3 |
| Tot. Data | 109 441 |
137 242 |
64 336 |
100 762 |
| Unique data | 9820 | 8078 | 5663 | 5731 |
| Observed data [I > 2.0 sigma(I)] | 8370 | 6436 | 3882 | 4256 |
| Rint | 0.058 | 0.106 | 0.183 | 0.045 |
| Completeness | 0.997 | 0.998 | 0.991 | 0.998 |
| Min. Resd. Dens./e Å−3 | −0.22 | −0.33 | −0.36 | −0.26 |
| Max. Resd. Dens./e Å−3 | 0.31 | 0.35 | 0.37 | 0.30 |
| Density/g cm−3 | 1.304 | 1.234 | 1.268 | 1.214 |
In H·o-Xy, the guest was disordered over two positions (with site occupancy factors (s.o.f.s) of 0.665(5) and 0.335(5)), while the crystals of the H·m-Xy inclusion compound were flexible, flat rods that were weakly diffracting, resulting in a high R value (0.1031). Additionally, one of the two guest molecules in the unit cell of H·2(p-Xy) also possessed positional disorder (s.o.f.s 0.749(7) and 0.251(7)), while the other guest species was not disordered.
The unit cells for guest-free H (Fig. 3a, top, a stereoview) and the H·o-Xy, (Fig. 3b, representing also isostructural H·m-Xy) and H·2(p-Xy) (Fig. 3c) complexes are also provided here. The host molecules in the crystals of each of guest-free H (Fig. 3a, bottom, also a stereoview) and H·2(p-Xy) (Fig. 3c) possessed an inversion of symmetry and, consequently, the two NH groups of the linker units were positioned in an antiperiplanar orientation (180.00°) with respect to one another. However, these molecules in the H·o-Xy and H·m-Xy complexes (which demonstrated an isostructural host packing motif) had these NH moieties in a more gauche orientation (66.61 and 66.08°). Moreover, after guest removal from the packing calculations and an analysis of the resulting spaces by means of a probe with a 1.2 Å radius, it was possible to prepare the void diagrams as demonstrated on the right-hand side in Fig. 3b and c. In all of these complexes, guests were accommodated in endless channels, unidirectional in the case of H·o-Xy and H·m-Xy (Fig. 3b) and bidirectional in the complex with p-xylene (Fig. 3c, with the disordered guest species in a different channel to the ordered guest molecules).
The close contacts that stabilized these crystalline forms were subsequently investigated. The packing of guest-free H did not involve any significant π⋯π interactions; however, two C–H⋯π contacts were identified in the unit cell, with H⋯π distances of 2.93 and 2.68 Å (C⋯π, 3.687(3) and 3.587(2) Å, 138 and 161°). Additionally, three nonclassical intermolecular hydrogen bonds of the C–H⋯O type were observed, involving the aromatic, methoxy or linker hydrogen atoms interacting with the oxygen atoms of the central xanthenyl B-ring or the methoxy moiety. These distances measured between 2.55 and 2.69 Å (H⋯O) and the applicable angles were 145–151°. Fig. 4(left) is an illustrative example, involving two methoxy moieties ((MeO)C–H⋯O–C(MeO), 2.55 Å, 148°). Finally, in these crystals was also noted a classical intermolecular hydrogen bond (Fig. 4, right): the amino hydrogen atom of the linker unit experienced a stabilizing close contact with the oxygen atom of a para-methoxy group of a neighbouring molecule with measurements 2.52(2) Å (H⋯O), 3.373(2) Å (N⋯O) and 155.9(18)°.
![]() | ||
| Fig. 4 Examples of nonclassical (left) and classical (right) intermolecular hydrogen bonds in the unit cell of guest-free H. | ||
As in guest-free H, no π⋯π close contacts were evident in the complex containing o-Xy. However, and again, C–H⋯π interactions were observed, both between host molecules (2.80–2.96 Å, 3.736(3)–3.807(3) Å, 149–168°) and between host and guest species, numbering two in the latter instance (Fig. 5), involving both disorder guest components, where the guest molecules served as the proton donors; here, measurements were 2.77 Å, 3.605(4) Å, 148° and 2.67 Å, 3.554(9), 155°. (The guest disorder over two positions is also clearly demonstrated in this figure). Moreover, the only classical hydrogen bonding in this complex was intramolecular in nature, serving to stabilise the geometry of each host molecule, between the hydrogen atom of the amino group of the linker unit and the second nitrogen atom of the same unit (2.61 Å (H⋯N), 2.945(3) Å (N⋯N) and 104°), while both intra- (C–H⋯N, 2.38 Å, 2.764(3) Å, 103° and 2.45 Å, 2.804(3), 102°) and intermolecular (C–H⋯O, 2.57 Å, 3.375(3) Å, 143°) nonclassical hydrogen bonds involving molecules of H were also identified.
Many similarities were noted in the noncovalent interactions present in H·o-Xy and H·m-Xy, expectedly, given the isostructural nature of their host packing. These include (host)C–H⋯π(host) (2.97–2.98 Å, 3.747(3)–3.899(3) Å, 138–166°) contacts as well as one (guest)C–H⋯π(host) (2.93 Å, 3.815(4) Å, 155°) intermolecular interaction. Once more, the conformation of the host molecule was stabilized by means of a singular intramolecular classical hydrogen bond involving the linker unit amino moieties (N–H⋯N, 2.55 Å, 2.914(5) Å, 106°), while the nonclassical hydrogen bonds were of the C–H⋯N (2.42 Å, 2.771(5) Å, 101° and 2.34 Å, 2.715(5) Å, 103°) and C–H⋯O (2.52 Å, 3.331(5) Å, 143°) types, as was the case in the o-Xy-containing inclusion complex.
In the case of H·2(p-Xy), which also did not experience any π⋯π contacts, an intermolecular (host)C–H⋯π(host) (2.96 Å, 3.692(2) Å, 133°) interaction involving a proton of the methoxy moiety and an aromatic ring of the xanthenyl system was identified. Furthermore, as was the occasion in the complexes with o-Xy and m-Xy, contacts of this type were also observed between host and guest species where the guest molecule was the proton donor; two such contacts were evident, measuring 2.96 Å, 3.710(7) Å, 133° and 2.67 Å, 3.582(17) Å, 161°, and involving only the two components of the disordered guest molecule and not the other non-disordered guest species, as illustrated clearly in Fig. 6. In fact, the ordered guest molecule was held in the crystals of the complex by means of steric factors only and no short contacts with the host species could be identified. Finally, the host molecule in this complex was not stabilized by an intramolecular classical N–H⋯N hydrogen bond, in contrast with this species in H·o-Xy and H·m-Xy. However, a singular intramolecular host C–H⋯N nonclassical bond of this type was identified (2.42 Å, 2.788(2) Å, 103°).
![]() | ||
| Fig. 6 The (guest)C–H⋯π(host) contacts involving only the two components of the disordered guest molecule and not the ordered guest species. | ||
Interestingly, these SCXRD data provide some insight into the selectivity behaviour of H during crystallization experiments from mixed guest solutions: all of the guest molecules in H·o-Xy and H·m-Xy, having guests that were more preferred, were retained in their channels through C–H⋯π contacts with the host compound, while not all of the p-Xy molecules (p-Xy being distinctly disfavoured by H) experienced this type of interaction (only the two disordered guest components were retained in this manner, and not the ordered guest molecules). Furthermore, the nature of the guest accommodation was also distinctly different: preferred o-Xy and m-Xy occupied unidirectional channels, while p-Xy was located in two channels in two separate orientations in its complex, one housing the ordered and the other the disordered guest molecules.
![]() | ||
| Fig. 7 Overlaid TG (red), DTG (green) and DSC (blue, endo up) traces for the inclusion complexes a) H·o-Xy, b) H·m-Xy and c) H·2(p-Xy). | ||
Each of the guest species in the three complexes was released in a distinct single-stepped process (Fig. 7a–c). Furthermore, the onset temperatures for this guest release event (Ton) in each of the three experiments were extremely comparable (41.7, 39.2 and 41.3 °C for H·o-Xy, H·m-Xy and H·2(p-Xy), respectively), suggesting that these inclusion compounds possess very similar relative thermal stabilities. This observation is not entirely surprising in the case of H·o-Xy and H·m-Xy since these complexes shared a host packing. These thermal data do not, as a result, provide a rationalization for the selectivity behaviour of H when presented with guest mixtures in that the more preferred guests did not form the more stable complexes, according to these data. However, as stipulated earlier, such explanations were clarified through the SCXRD experiments.
:
G ratios of the three successfully furnished complexes were 1
:
1, 1
:
1 and 1
:
2 (o-Xy, m-Xy and p-Xy). When H was crystallized from guest solutions, a host selectivity order of o-Xy > EB > m-Xy > p-Xy was noted. In fact, it was shown that H may serve to purify EB and m-Xy solvents when contaminated with small quantities of o-Xy and EB, respectively. SCXRD experiments demonstrated that more preferred o-Xy and m-Xy always experienced a (guest)C–H⋯π(host) close contact with H, facilitating guest retention, while not all of the guest molecules in H·2(p-Xy) were involved in these types of stabilizing interactions with the host species, thus explaining the low preference of H for p-Xy. The relative thermal stabilities of the three single solvent complexes were, moreover, established to be equivalent through thermoanalytical experiments since Ton, the onset temperatures of the guest release events, ranged between only 39.2 and 41.7 °C.
Supplementary information (SI): the relevant ORTEP diagrams and 1H-NMR spectra may also be found in this section. See DOI: https://doi.org/10.1039/d6ce00160b.
CCDC 2530251–2530254 (H, H·o-Xy, H·m-Xy and H·2(p-Xy)) contain the supplementary crystallographic data for this paper.46
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