Tropylium cation capsule of hydrogen-bonded tetraurea calix[4]arene dimers

Limor Frish a, Myroslav O. Vysotsky b, Susan E. Matthews b, Volker Böhmer *b and Yoram Cohen *a
aSchool of Chemistry, The Sackler Faculty of Exact Sciences, Tel Aviv University, Ramat Aviv 69978, Tel Aviv, Israel
bFachbereich Chemie und Pharmazie, Abteilung Lehramt Chemie, Johannes-Gutenberg-Universität, Duesbergweg 10-14, D-55099 Mainz, Germany

Received (in Cambridge, UK) 5th September 2001 , Accepted 22nd October 2001

First published on 26th November 2001


Abstract

The interaction between tropylium salts and tetraurea calix[4]arene derivatives (such as 1 and 2) was studied in solution using 1D, 2D, diffusion, VT NMR and UV–visible spectroscopy. It was found that tropylium salts form charge transfer complexes with both the monomers and dimers of the tetraurea calix[4]arene derivatives depending on the experimental conditions. Compound 1 increases dramatically the solubility of tropylium salts in apolar solvents such as C2D4Cl2, CDCl3 and CD2Cl2 by forming the molecular capsule 1·C7H7+·1. In contrast to the benzene capsule of 1, in 1·C7H7+·1 the hydrogen bonds in the equatorial region that hold together the two parts of the dimer change their directionality faster than the NMR time scale (at 400 MHz) at temperatures higher than 298 K. Interestingly, the free energy barrier for this dynamic process at 298 K (ΔG298), depends on the nature of the counter-anion. Free energies of activation of 14.3 ± 0.2 kcal mol−1 and 12.6 ± 0.2 kcal mol−1 were found by total lineshape analysis for the dimeric capsules of C7H7+PF6 and C7H7+BF4, respectively. The affinity of the tropylium cation toward the dimer's cavity is much higher than that of neutral organic guests. Although exact quantitative values are not available due to the low solubility of tropylium salts in apolar solvents, a rough estimation in CD2Cl2 shows that the tropylium cation affinity is several orders of magnitude higher than that of benzene, which is known to be a good guest. These results show that once the steric requirements are met, electronic effects may serve as an additional driving force for the formation of such molecular capsules demonstrating the importance of cation–π interactions in such systems.


Introduction

Molecular capsules in general1 and those obtained by dimerization of tetraurea calix[4]arene derivatives in particular have attracted much interest in recent years.2,3 These dimers, held together in non-polar solvents by a belt of hydrogen bonds between the urea functions, were studied in the solid state by X-ray crystallography4 and in solution by 1D and 2D NMR.2,3,5 With tetraalkylammonium cations as guests, electrospray mass spectrometry (ES-MS) could be also used to characterize the structure of such capsules.6 Previously, we demonstrated that diffusion measurements using the pulsed gradient spin echo (PGSE) technique7 provide a means of following molecular interactions in solutions.8 Consequently, this technique was used to study the dimerization, encapsulation and the disruption of tetraurea calix[4]arene dimers in solutions.8e

Mostly steric effects such as size or shape were considered when discussing the relative affinity of various guests towards the cavity of the capsules. In the absence of stronger and more specific interactions such as hydrogen bonding or cation–π interactions a packing coefficient of 55%, as is found for many organic solvents, seems to be ideal for the inclusion of “molecules within molecules”.9 However, many exceptions in both directions have been found for dimers of tetraurea calix[4]arenes. Among neutral guests pyrazine (38%) and benzene (38%) are accepted as well as nopinone (71%) or myrtenol (76%).6 The occupation of 78% of the capsule volume (if this is taken as 190 Å3) by the tetraethylammonium cation may be due to its stronger interaction with the π-basic cavities.10

It was suggested that cation–π interactions play an important role in several biological systems.11 Recently we were able to show that the formation of a dimeric capsule from resorcarene tetraesters could be induced by tropylium cations.12a Thus, we decided to study the molecular interaction between tetraurea calix[4]arenes and the tropylium cation which has the additional intrinsic advantage that the interaction with the calixarene host is also indicated in the UV spectrum by charge transfer bands, as in other cases.12b,c

Results and discussion

Addition of a tropylium salt to the colorless solution of tetraurea calix[4]arenes 1 (Scheme 1) results in a deep red solution indicative of the formation of a charge transfer complex. This coloration occurs in apolar as well as in polar solvents.
scheme, filename = b108043a-s1.gif
Scheme 1

NMR studies of tropylium complexation

In apolar solvents having the “wrong” shape or size,9 such as CD2Cl2, tetraurea derivative 1 forms only ill defined aggregates as suggested by the broad signals in the 1H NMR spectrum of 1 for example.5 However, addition of small amounts of a suitable guest, such as benzene, induces the formation of a well defined species characterized by narrow signals in the 1H NMR spectrum.5 Similar observations were made for the addition of a tropylium salt (Fig. 1) where an even smaller amount is needed to induce the complete formation of a well-defined species in CD2Cl2. This suggests that the interaction between the tropylium cation and 1 is stronger than that between 1 and benzene.
The aromatic region of the 1H NMR spectrum (500 MHz) of tetraurea calix[4]arene 1 in CD2Cl2 (at C = 5 × 10−3 M) at room temperature (A) and after saturation with tropylium hexafluorophosphate (B).
Fig. 1 The aromatic region of the 1H NMR spectrum (500 MHz) of tetraurea calix[4]arene 1 in CD2Cl2 (at C = 5 × 10−3 M) at room temperature (A) and after saturation with tropylium hexafluorophosphate (B).

Additional support for the interaction between tetraurea calix[4]arenes 1 and tropylium cations is gained from the observation that a second set of signals appears in the 1H NMR spectrum when small amounts of a tropylium salt are added to a solution of 1 in an organic solvent such as C2D4Cl2 where tetraurea calix[4]arenes are known to form dimers. As one set of signals represents the dimer with an encapsulated solvent molecule (i.e. C2D4Cl2) the second set of signals should be attributed to the species bound to tropylium, probably to the tropylium capsule (Fig. 2).


The aromatic region of the 400 MHz 1H NMR spectrum of tetraurea calix[4]arene 1 in C2D4Cl2 at room temperature (A) in the absence, and (B) in the presence of a small amount of tropylium hexafluorophosphate.
Fig. 2 The aromatic region of the 400 MHz 1H NMR spectrum of tetraurea calix[4]arene 1 in C2D4Cl2 at room temperature (A) in the absence, and (B) in the presence of a small amount of tropylium hexafluorophosphate.

The fact that in apolar solvents the charge transfer complex of tropylium cation and 1 is a dimeric capsule was established by a combination of NMR measurements and by UV–visible spectroscopy. For 1·C7H7+·1 one should expect two doublets for He,f (Scheme 1) and four additional signals in the aromatic region of the 1H NMR spectrum; two singlets should represent the two NH groups (Ha,b, Scheme 1), and the two aromatic protons (Hc,d, Scheme 1) known to be chemically non-equivalent in capsules filled with benzene, chloroform etc. should show two meta-coupled doublets. The encapsulated tropylium cation should appear upfield shifted with respect to its usual position. However, only three and not five signals are found at 298 K in the aromatic region of the 1H NMR spectrum of the complex formed between 1 and tropylium hexafluorophosphate in C2D4Cl2 (Fig. 3) or CD2Cl2 (Fig. 1B) in addition to the AA′BB′ system attributed to He,f. Only when the 1H NMR spectrum is recorded at lower temperatures is the expected pattern found and the two broad signals at 5.6 and at 7.4 ppm became clearly apparent (see below). Such changes in the 1H NMR spectrum were observed in CD2Cl2, CDCl3 and C2D4Cl2 solutions of 1 and tropylium salts (Fig. 3).


The aromatic region of the 400 MHz 1H NMR spectrum of 1·C7H7+·1 in C2D4Cl2 (solution of 1 saturated with C7H7+ PF6−) as a function of the temperature.
Fig. 3 The aromatic region of the 400 MHz 1H NMR spectrum of 1·C7H7+·1 in C2D4Cl2 (solution of 1 saturated with C7H7+ PF6) as a function of the temperature.

The assignment of the 1H and 13C NMR spectra of the dimeric capsule 1·C7H7+·1 in C2D4Cl2 was obtained by a series of 2D NMR experiments performed at low temperature. First, the DQF-COSY 1H NMR spectrum of this complex at 258 K showed a clear correlation only between the two signals at 5.6 ppm and 7.4 ppm suggesting that they belong to the two meta-coupled aromatic protons Hc,d. The HMQC spectrum revealed correlations between the protons at 5.6 and 7.4 ppm and the carbons at 126.0 and 126.7 ppm, respectively and a correlation between the proton at 5.4 ppm and the carbon at 160 ppm. No correlations could be found between the protons at 8.8 and 6.9 ppm and any carbon suggesting that these singlets represent the two protons of the NH groups (Scheme 1). Based on these observations we assigned the singlet at 5.4 ppm to the encapsulated tropylium cation. Indeed, a phase-sensitive NOESY experiment performed at 258 K on the C2D4Cl2 solution of the complex revealed strong correlations between the two meta-coupled doublets and four out of the five signals, while the peak at 5.4 ppm showed only very weak correlations with the signals at 5.6 ppm and 7.4 ppm. This is to be expected since intramolecular NOEs are known to be much stronger than intermolecular NOEs. The large high field shift of 3.8 ppm thus observed for the complexed tropylium cation is in line with its encapsulation in the dimer 1·1,13 since a smaller shift would be expected for its inclusion in the monomeric 1.12a For the encapsulated benzene in the dimer 1·1 a high field shift of 2.7 ppm was reported.5

Further evidence for the dimeric nature of this complex comes from diffusion measurements performed on the tropylium cation complex of 1 in C2D4Cl2 solution at low temperatures. In this experiment we found that all the peaks at the aromatic region of the 1H NMR spectrum, including the signal at 5.4 ppm, have the same diffusion coefficients within experimental errors (Fig. 4). This means that the tropylium cation and the tetraurea calix[4]arene 1 diffuse as one supramolecular entity. In addition, the diffusion coefficients of the signals of the tropylium cation complex of 1 and 1·C6D6·1 in C6D6 solutions8e were found to be equal, within experimental errors (0.30(±0.01) × 10−5 cm2 s−1 and 0.32(±0.01) × 10−5 cm2 s−1, respectively.) (Fig. 5). These observations support the conclusion that the tropylium cation is included in a dimeric capsule like the benzene.


The natural log of the normalized signal attenuation (ln I/I0) as a function of the b values19 for all the five signals observed in the aromatic region of the 1H NMR spectrum of 1·C7H7+·1 in C2D4Cl2 at 258 K, including the singlet at 5.4 ppm attributed to encapsulated tropylium cation (●) and the peak of C2D4Cl2 (■).
Fig. 4 The natural log of the normalized signal attenuation (ln I/I0) as a function of the b values19 for all the five signals observed in the aromatic region of the 1H NMR spectrum of 1·C7H7+·1 in C2D4Cl2 at 258 K, including the singlet at 5.4 ppm attributed to encapsulated tropylium cation (●) and the peak of C2D4Cl2 (■).


            1H NMR spectra of the Stejskal and Tanner diffusion experiment in C6D6 solution showing the signal intensity decay as a function of the pulsed gradient strength (G) of (A) 1·C6D6·1, and (B) 1·C7H7+·1. For clarity only the signal decay of the peaks at 6.39 and 6.19 ppm of 1·C6D6·1 and 1·C7H7+·1, respectively
are shown.
Fig. 5 1H NMR spectra of the Stejskal and Tanner diffusion experiment in C6D6 solution showing the signal intensity decay as a function of the pulsed gradient strength (G) of (A) 1·C6D6·1, and (B) 1·C7H7+·1. For clarity only the signal decay of the peaks at 6.39 and 6.19 ppm of 1·C6D6·1 and 1·C7H7+·1, respectively are shown.

Finally, the formation of a dimeric capsule with included tropylium cation was proved, as in other cases, by the formation of heterodimers. The 1H NMR spectrum of a mixture of two different tetraurea calix[4]arenes (1 and 3, Scheme 1) in the presence of tropylium hexafluorophosphate shows not only the signals found in the spectra obtained separately for each derivative, as expected for monomeric complexes with tropylium. It clearly reveals the presence of a third species with lower symmetry (Fig. 6). The only plausible explanation for these observations is the formation of a heterodimer 1·C7H7+·3 in addition to the two homodimers 1·C7H7+·1 and 3·C7H7+·3.


Sections of the 400 MHz 1H NMR spectra of tetraureacalix[4]arene derivatives in the presence of tropylium hexafluorophosphate in CD2Cl2 at 298 K, (A) a mixture of 3 and 1, (B) 3, and (C) 1.
Fig. 6 Sections of the 400 MHz 1H NMR spectra of tetraureacalix[4]arene derivatives in the presence of tropylium hexafluorophosphate in CD2Cl2 at 298 K, (A) a mixture of 3 and 1, (B) 3, and (C) 1.

Two meta-coupled doublets for the aromatic protons (Hc,d) are observed, if the directionality of the hydrogen bonded belt is “fixed on the NMR-time scale” (S8-symmetry of the dimer); however, if the change in the directionality of the hydrogen bonds is rapid on the NMR time scale a single singlet (due to the D4d-symmetry of the dimer) should be expected for those protons.10 From the total lineshape analysis of the variable temperature 1H NMR spectra as those reported in Fig. 3 we could extract for this rotation, at 298 K, an energy barrier of ΔG = 14.3 ± 0.2 kcal mol−1 and ΔG = 12.6 ± 0.2 kcal mol−1 for 1·C7H7+·1 when the counter-anions were PF6 and BF4, respectively.14

For steric reasons it can be excluded that the anions (PF6 or BF4) are also encapsulated by the dimer,15 while it is not clear if these anions interact with the molecular capsule from the outside. To get some insights concerning the interaction of PF6 and BF4 with 1·C7H7+·1 in the solution, we have measured the 19F NMR of these tropylium salts in C2D4Cl2 in the presence and in the absence of 1. Interestingly, we found no changes in the chemical shifts and the lineshape of the 19F NMR in the case of C7H7+PF6 upon addition of 1; however, a pronounced lineshape change was observed for the C7H7+BF4 case. These results may suggest that BF4 interacts more significantly than PF6 with the tropylium encapsulated dimer and may explain the larger assistance of BF4, which results in a lower energetic barrier for the rotation of the hydrogen bond belt of 1·C7H7+·1. In addition, we have measured the diffusion coefficient of PF6 using 31P diffusion NMR spectroscopy on a more concentrated solution of 1 and C7H7+PF6 in C2D4Cl2. The diffusion coefficient of PF6 was found to be much higher than that of the encapsulated tropylium (0.73(±0.09) × 10−5 cm2 s−1 and 0.21(±0.01) × 10−5 cm2 s−1, respectively). Due to the relatively low solubility of C7H7+PF6 in C2D4Cl2 we could not measure the diffusion coefficient of PF6 in the absence of 1. However, the large difference between the diffusion coefficients of the dimer and the PF6 suggests that there is very little, if any, interaction between the two species under these experimental conditions. Basically the C7H7+PF6 ion pair behaves as a solvent separated ion-pair in C2D4Cl2 in the presence of 1. Assuming a spherical shape for the dimer and the PF6 the ratio between their diffusion coefficients should be inversely proportional to the cubic root of their molecular weights ratio. Therefore one should expect a ratio of 2.8 between the diffusion coefficients of PF6 and 1, while experimentally a ratio of 3.5 was found.

From the results presented so far it is clear that tropylium cations have a much stronger tendency to induce the formation of dimeric capsules, than neutral organic templates. Unfortunately, we could not characterize this “tendency” in a more quantitative way by giving template ratios.16 Many of the solutions of 1·C7H7+·1 PF6 and other competing neutral guests in apolar solvents were unstable over a period of 1–4 weeks. During this time precipitate is formed and one (in CD2Cl2) or two (in CDCl3, see below) additional sets of signals are observed. The relative integral intensities of all signals continuously change and we could never reach quantitatively the same situation starting either from the complex 1·C7H7+·1 adding a neutral guest or from separate components (1, C7H7+PF6, neutral guest and non-competing solvent), which of course would be the best proof that the thermodynamic equilibrium is reached.

The addition of ∼10% DMSO-d6 to a solution of 1·C7H7+·1 in an apolar solvent disrupts the capsule as shown by the 1H NMR spectrum, e.g. by the disappearance of the singlet at 5.4 ppm attributed to the encapsulated tropylium cation. A concentration dependent peak between 7.0 and 9.0 ppm for C7H7+ shifted to high field for increasing [1] and to low field for increasing [C7H7+] is characteristic for a time-averaged situation for free C7H7+ (9.2 ppm in C2D4Cl2 with 10% DMSO-d6) and its complex with monomeric 1. Consequently, the downfield shift of this peak is accompanied by a gradual increase in the extracted diffusion coefficient. The red colour of C2D4Cl2 solutions of C7H7+ and tetraurea 4, which for steric reasons cannot form dimers, is an additional indication of the interaction of the tropylium cation with the monomeric tetraureas.

UV–vis studies of tropylium complexation

The complex 1·C7H7+·1 PF6, prepared in dichloromethane by extraction of C7H7+·PF6 into the solution of 1, filtration from excess salt and subsequent evaporation, can be easily dissolved in a range of apolar solvents like dichloromethane, 1,2-dichloroethane and chloroform forming red solutions. The spectra recorded in dichloromethane and dichloroethane are very similar with two very broad bands at about 344 and 491 nm, indicating a charge transfer interaction between the included tropylium cation and benzene rings of the calixarene dimer. Similar UV–vis spectra with two very broad bands (at λ 339.3 and 415.5 nm in acetonitrile) have been observed for the tropylium complex with dibenzo-24-crown-8.12b The red shift especially for the second band reflects a smaller energy gap for the charge transfer process for the 1·C7H7+·1 PF6 complex due to, most probably, a stronger interaction between the tropylium cation and the dimeric capsule of 1. All absorption bands follow the Lambert–Beer law in the concentration range of 1.0–0.02 mM, which proves that no detectable dissociation occurs.

The spectra recorded in chloroform show an additional shoulder at 405.5 nm (Fig. 7). This might be caused by the presence of a complex of monomeric 1 with tropylium cation (see below) under these conditions. In fact, the 1H NMR spectrum of the complex 1·C7H7+·1 PF6 dissolved in CDCl3 (Fig. 8), clearly reveals two additional sets of calixarene signals. The first is due to the complex 1·CDCl3·1 and the second most probably due to the complex 1·C7H7+·PF6, which is in fast exchange with the monomer of 1. This would explain why, under these conditions, signals for the free tropylium are not observed. A small amount of a white precipitate is attributed to the tropylium salt C7H7+·PF6.


The UV–vis spectra of the 1·C7H7+·1 PF6− complex recorded in two different solvents at 2.71 × 10−4 M concentration.
Fig. 7 The UV–vis spectra of the 1·C7H7+·1 PF6 complex recorded in two different solvents at 2.71 × 10−4 M concentration.

The 1H NMR spectrum of the complex 1·C7H7+·1 PF6− dissolved in CDCl3 (c
≈ 7 mM). In addition to the signals of the 1·C7H7+·1 PF6− (●), signals for 1·CDCl3·1 (○) and a third species (*) can be distinguished.
Fig. 8 The 1H NMR spectrum of the complex 1·C7H7+·1 PF6 dissolved in CDCl3 (c ≈ 7 mM). In addition to the signals of the 1·C7H7+·1 PF6 (●), signals for 1·CDCl3·1 (○) and a third species (*) can be distinguished.

If increasing amounts of DMSO are added to the 1,2-dichloroethane solution of the complex first a decrease of the absorption at 344 and 491.5 nm and a simultaneous increase at ∼400 nm is observed (Fig. 9). For DMSO contents of more than 3% a general decrease of the absorption in the whole 320–500 nm range is observed. This can be reasonably explained by a dissociation of the 2 ∶ 1 complex via the 1 ∶ 1 complex into the monomeric urea and the tropylium cation with increasing polarity of the solvent mixture. A Job plot in 1,2-dichloroethane (Fig. 10a) unequivocally proves the 2 ∶ 1 (host ∶ guest) stoichiometry of the complex under these conditions, which is in line with the NMR data. For the mixture of 1,2-dichloroethane with 25% of DMSO the maximum in the Job plot is observed at 1 ∶ 1 (1: C7H7+PF6, Fig. 10b) ratio, in agreement with a complete dissociation of the dimer and the formation of a tropylium complex with the monomeric tetraurea calix[4]arene. These results are completely in line with the 1H NMR results, which were discussed previously and were depicted in Figs. 1 and 2.


UV–vis spectra of the 1·C7H7+·1 PF6− complex recorded in 1,2-dichloroethane at 2.42 × 10−4 M concentration with different amounts of DMSO.
Fig. 9 UV–vis spectra of the 1·C7H7+·1 PF6 complex recorded in 1,2-dichloroethane at 2.42 × 10−4 M concentration with different amounts of DMSO.

Job plots obtained for the urea 1 and C7H7+PF6− in (A) 1,2-dichloroethane (at c
= 7.84 × 10−4 M) and (B) in 1,2-dichloroethane with 25% of DMSO (at c
= 5.70 × 10−3 M).
Fig. 10 Job plots obtained for the urea 1 and C7H7+PF6 in (A) 1,2-dichloroethane (at c = 7.84 × 10−4 M) and (B) in 1,2-dichloroethane with 25% of DMSO (at c = 5.70 × 10−3 M).

While the complex 1·C7H7+·1 PF6, is not sufficiently soluble in cyclohexane it dissolves in solvents like benzene and isopropanol, however the initial red color disappears almost immediately. Most probably this is due to the complete substitution of the included tropylium cation by benzene in the first case and to the complete dissociation of the dimeric capsules in the latter case.17 In tetrachloromethane the color disappears within 20–30 minutes18 which offers the possibility of following kinetically the exchange of the included tropylium cation by the solvent molecules. First experiments show, however, that the rate law is obviously not of the expected pseudo-first order.

Conclusion

We have demonstrated that tetraurea calix[4]arenes form molecular capsules in apolar solvents with the tropylium cation included in the cavity formed by this dimerization. The relative affinity of the tropylium cation towards the tetraurea calix[4]arene cavity 1 is at least several orders of magnitude larger than that of benzene which has a similar size. The directionality of the belt of hydrogen bonded urea groups holding the two parts of the dimer changes relatively fast at 400 MHz above room temperature. The energy barrier for this dynamic process was found to be anion dependent. These results prove that electronic effects play a decisive role in determining the relative affinity of C7H7+ toward the capsule cavity. UV and NMR data demonstrate that tropylium cations interact also with 1 in its monomeric form.

In summary these results suggest that once the steric requirements are met electronic interactions can be used to drive the formation of such molecular capsules. These data provide an additional example for the importance of cation–π interactions in such systems.

Experimental

Materials

All the deuterated solvents were supplied by Aldrich (USA) and used as is. The tetraurea calix[4]arene derivatives were prepared according to the procedure published in references 2c, d.

Complexation

Since tropylium salts are poorly soluble in most organic solvents, solutions of tropylium capsules in various solvents were prepared by treating the tetraurea calix[4]arene and a slight excess of the tropylium salt with dichloromethane or 1,2-dichloroethane, followed by filtration, evaporation and addition of the desired deuterated solvent.
1H NMR of 1·C7H7+·1 PF6 (400 MHz, 298 K, C2D4Cl2). δ = 8.75 (s, 8H), 7.53 (d, J = 7.9 Hz, 16H), 7.4 (broad, 8H), 7.14 (d, J = 7.9 Hz, 16H), 6.91 (s, 8H), 5.6 (broad, 8H), 5.35 (s, 7H), 4.28 (d, J = 12 Hz, 8H), 3.71 (m, 16H), 2.82 (d, J = 12 Hz, 8H), 2.21 (s, 24H), 1.89 (m, 16H), 1.24 (m, 112H), 0.82 (t, J = 6.2 Hz, 24H).
1H NMR of 1·C7H7+·1 PF6 (400 MHz, 258 K, C2D4Cl2). δ = 8.80 (s, 8H), 7.55 (d, J = 7.9 Hz, 16H), 7.45 (s, 8H), 7.15 (d, J = 7.9 Hz, 16H), 6.94 (s, 8H), 5.64 (s, 8H), 5.29 (s, 7H), 4.25 (d, J = 12 Hz, 8H), 3.68 (m, 16H), 2.83 (d, J = 12 Hz, 8H), 2.23 (s, 24H), 1.91 (m, 16H), 1.23 (m, 112H), 0.83 (t, J = 6.2 Hz, 24H).

NMR measurements

NMR spectra were recorded on 500 MHz ARX and 400 MHz Avance Bruker NMR spectrometers (Karlshruhe, Germany). The solvents were used as internal lock and internal references (1H NMR: C6D6 7.15 ppm, CD2Cl2 5.3 ppm, C2D4Cl2 3.65 ppm, CDCl3 7.26 ppm; 13C NMR: C6D6 128.7 ppm, C2D4Cl2 51.7 ppm, CDCl3 77.0 ppm). Diffusion experiments were carried out on the 500 MHz NMR spectrometer equipped with a B-AFPA 10 pulsed gradient unit capable of producing Z-gradient of about 50 G cm−1 or on the 400 MHz NMR spectrometer equipped with a Great 1/10 pulse gradient unit capable of producing Z-gradient of about 50 G cm−1. All experiments were carried out in a 5 mm inverse probe using a 4 mm NMR tube inserted in a 5 mm NMR tube. All 1H diffusion measurements were performed with a PGSE pulse sequence7 with pulse gradient duration of 2 ms and a pulsed gradient separation of 62 ms. The pulsed gradients were incremented from 0 to 46.8G cm−1 (in the 500 MHz instrument) or to 40.2G cm−1 (in the 400 MHz instrument) in ten steps. The diffusion experiments were preformed at least three times and in the 1H NMR diffusion experiment only data for which the correlation coefficient was higher than 0.999 were included. In the 31P NMR diffusion experiments due to the lower signal to noise the correlation coefficients were only 0.995.

UV–vis studies

All spectra were measured with a Jasco V-530 instrument at 22 °C using 1 cm cuvettes.

Acknowledgements

Financial support from the Deutsche Forschungsgemeinschaft (BO 523/14-1) and the Israel Science Foundation (ISF) is gratefully acknowledged.

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  14. A similar dependence of the counter-anion was observed for tetraethylammonium as guest, and is presently studied more in detail.
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  16. The template ratios Kr which are usually defined as the ratio of the stability constants K of the (self-assembled) complexes. 21 + G ⇆ 1·G·1 with K = [1·G·1]/([G][1]2) and Kr = K1/K2 = ([1·G1·1] [G2])/([G1] [1·G2·1]). This new constant Kr can be understood also as the equilibrium constant for the exchange reaction: [G1] + [1·G2·1] ⇆ [G2] + [1·G1·1] To determine Kr the ratio [1·G1·1]/[1·G2·1], which follows from the integration of analogous peaks of the two complexes, and the ratio [G1]/[G2], both usually applied in excess to 1, must be known. In the present case the situation is further complicated by the low solubility of tropylium salts in apolar solvents and at the moment we can only give an estimate for the lower limit for Kr. If C6D6 (= G2) is added to a 1.87 mM solution of 1·C7H7+·1 in CD2Cl2 (a solvent which does not induce the dimerization) up to [C6D6] = 3.66 M the NMR spectrum showed only small changes in the chemical shifts, but signals for 1·C6D61·could not be detected. (The solution shows no changes within several days, while a precipitate occurs after weeks). Thus, the ratio [1·G2·1]/[1·C7H7+·1] should be lower than 0.1 (under the surely not too optimistic assumption that 10% of an additional dimer would be detected), and for the same reason the actual ratio [C7H7+]/[C6D6] should be less than (0.1 × 1.87 × 10−3)/3.66). Therefore, under these experimental conditions Kr > 2 × 105.
  17. In these cases the tropylium salt precipitated from the solution what was observed by appearance of turbidity of the solutions with following formation of a white crystalline powder.
  18. A similar behavior is observed for toluene solutions.
  19. The diffusion coefficients were determined by the PGSE technique according to which the ratio between the echo intensity in the presence (I) and in the absence of pulsed gradient (I0) is given by eqn. (1)7 in which γ is the gyromagnetic ratio, g is the pulsed gradients strength, Δ and δ are the time separation between the pulsed-gradients and their duration, respectively and D is the diffusion coefficient. For an isotropic solution, a plot of ln(I/I0) vs.b should give a straight line which slope is equal to −D.7
     
    ln (I/I0) = −γ2g2δ2(Δδ/3)D = −bD(1)
    .

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