Ken Cham-Fai Leung*ab, Wing-Yan Wonga, Fabio Aricób, Philip C. Haussmannb and J. Fraser Stoddart*bc
aCenter of Novel Functional Molecules, Department of Chemistry, The Chinese University of Hong Kong, Shatin, NT, Hong Kong SAR, P. R. China. E-mail: cfleung@cuhk.edu.hk; Fax: (+852) 2603-5057
bCalifornia NanoSystems Institute and Department of Chemistry and Biochemistry, The University of California, Los Angeles, 405 Hilgard Avenue, Los Angeles, California 90095, USA
cDepartment of Chemistry, Northwestern University, 2145 Sheridan Road, Evanston, Illinois 60208, USA. E-mail: stoddart@northwestern.edu; Fax: (+1) 847-491-1009
First published on 20th November 2009
Large amounts (>100 mol equivalents) of water are required to effect by hydrolysis the partial disassembly of the rings from the dumbbell components of two dynamic [2]rotaxanes. The two dynamic [2]rotaxanes are comprised of [24]crown-8 rings—each of which incorporate two imine bonds—encircling a dumbbell component composed of a dibenzylammonium ion in which each of the two benzyl substituents carries two methoxyl groups attached to their 3- and 5-positions. A mechanism for the partial disassembly of the two dynamic [2]rotaxanes, involving the cleavage of the kinetically labile imine bonds by water molecules, is proposed. The most important experimental observation to be noted is the fact that the hydrolysis of the macrocyclic diimines, associated with the templating –CH2NH2+CH2–centres in the middle of their dumbbells, turns out to be an uphill task to perform in the face of the molecular recognition provided by strong [N+–H⋯O] hydrogen bonds and weaker, yet not insignificant, [C–H⋯O] interactions. The dynamic nature of the imine bond formation and hydrolysis is such that the acyclic components produced during hydrolysis of the imine bonds can be enticed to cyclise once again around the –CH2NH2+CH2–template, affording the [2]rotaxanes. The reluctance of imine bonds, present in substantial numbers in larger molecular and extended structures, is significant when it comes to exercising dynamic chemistry in compounds where multiple imine bonds are present.
Generally, imines are relatively unstable since they are susceptible to rapid hydrolysis in the presence of water.9 Saggiomo and Lüning10 have reported recently, however, that imine-containing macrocycles possess remarkable stabilities in the presence of water. Other molecular systems,11 involving dative bonds between imines and transition metal ions,12 can also experience increased imine stabilities in water. It follows that a careful investigation of the dissociative mechanisms associated with the formation and hydrolysis of dynamic rotaxanes containing imine bonds is important in the context of the design of functional rotaxanes13 that can be obtained in high yields by DCC and possess potentially useful applications.14
In this paper, we report an investigation of the dissociation of dynamic, imine-containing rotaxanes8a in the presence of an excess of water. It transpires that not only is the hydrolysis far from complete, but also that the dissociated molecular components obtained at equilibrium can be assembled rather easily to afford the original [2]rotaxanes by removing the water from the aqueous solutions with appropriate drying agents.
:
1
:
1 ratio—the diformylpyridine 2, the diamine 3a and the already stoppered dialkylammonium salt 4–H·PF6—in dry MeCN (60 mM) in over 90% yield in one pot. Similarly, another dynamic [2]rotaxane 1b–H·PF6 can also be formed using the same condensation method with 2, the diamine 3b and 4–H·PF6 in a 1
:
1
:
1 ratio. Moreover, we found out experimentally that the condensations occur effectively in both MeCN and MeNO2 (60 mM). The encirclement of a dialkylammonium ion by the imine-containing [24]crown-8 macrocycle can be regarded as a thermodynamically controlled template-directed self-assembly and amplification process. Since the dialkylammonium ion template 4–H·PF6 fits well into the macrocycle, which is generated from the [1 + 1] condensation between 2 and 3a/b, the [2]rotaxanes 1a/b–H·PF6 can be amplified as the major products in the dynamic competitive equilibrium mixture. Subsequently, the [2]rotaxanes 1a/b–H·PF6 were characterised by 1H NMR spectroscopy and matrix-assisted laser-desorption ionization mass spectrometry (HR-MALDI-MS) (mass spectra not shown). The 1H NMR spectra were obtained after 15 min of mixing between the free components. The 1H NMR spectra of the dynamic [2]rotaxanes reveal that the characteristic benzylic methylene proton signals, adjacent to the ammonium ion centre, observed at 3.8–3.9 ppm of 4–H·PF6 are shifted downfield to 4.5–4.6 ppm upon rotaxane formation. Moreover, the characteristic peaks for the protons on the ethyleneglycol chain are shifted upfield (see the ESI†). The [2]rotaxanes are stable entities on account of [N+–H⋯O] and [N+–C–H⋯X] (X
O or N) hydrogen bonds, in addition to electrostatic and π–π stacking interactions.8c Thereafter, they were redissolved in MeCN prior to carrying out dissociation studies in the presence of different amounts of water.![]() | ||
| Scheme 1 Equilibrium for the self-assembly and dissociation of the dynamic [2]rotaxanes 1a/b–H·PF6 and their components 2, 3a/b and 4–H·PF6 depending on the concentration of water present in the reaction mixture. | ||
Our investigations have shown that the dissociation of dynamic [2]rotaxanes 1a/b–H·PF6 requires large amounts of water. Thus, 1H NMR spectroscopy was employed for investigating the dissociation of 1a/b–H·PF6, following addition15 of 100, 200, 250 and 500 equivalents of D2O. Whether or not equilibration has been reached, sharp signals in the 1H NMR spectra of the [2]rotaxanes indicate that they are relatively stable kinetically on the NMR timescale at 500 MHz. The stability is presumably the result of the stabilizing multiple noncovalent bonding interactions. By way of an example, Fig. 1 shows the stacked 1H NMR spectra (500 MHz, CD3CN, 298 K, aromatic region, 16.6 mM, b = bound rotaxane and f = free components) of the [2]rotaxane 1a–H·PF6 in the presence of 200 equivalents of D2O. Initially, the NMR spectra of [2]rotaxane 1a–H·PF6 (at 0 min) reveal the proton signals at δ = 7.71 ppm and δ = 8.02 ppm for the bound (b) pyridine ring, at δ = 6.9–7.5 ppm for the bound (b) N,O-substituted aryl ring, and at δ = 6.10 ppm and δ = 6.45 ppm for the bound (b) dimethoxyaryl ring. With increasing time in the presence of water, the characteristic proton signals originating from the aldehyde (δ = 10.12 ppm), the free (f) pyridine ring (δ = 8.22 ppm) and the free (f) dimethoxyaryl ring (δ = 6.58 and 6.62 ppm) in separate cyclic (or acyclic) and dumbbell components were found to have their relative intensities increase, while those signals arising from the rotaxane decreased. The low intensity aldehyde signal at 10.10 ppm can be attributed to the intermediate monoaldehyde 5a/b formed during the hydrolysis of 1a/b–H·PF6. The results indicate that the dynamic [2]rotaxane dissociates slowly into its free components—2, 3a and 4–H·PF6—until the dissociation process has reached equilibrium after 24 h. Furthermore, the broad signal (δ = 9.98 ppm) for the NH2+ centre became diminished with time on account of proton/deuterium exchange. With particular reference to 1a–H·PF6, there were 52, 41 and 14% of the dynamic [2]rotaxane remaining in the mixture after 24 h following the additions, in turn, of 100, 200 and 500 equivalents of D2O. On the other hand, in the case of the dissociation of 1b–H·PF6, there were 19, 8 and 4% of the dynamic [2]rotaxane remaining in the mixture after 24 h following the additions, in turn, of 100, 250 and 500 equivalents of D2O. Moreover, the 1H NMR spectra reveal that the residual dynamic [2]rotaxanes 1a/b–H·PF6 are stable in the CD3CN–D2O mixture after 24 h, reflecting a situation that is able to maintain the integrity of the [2]rotaxane constitution, even in the presence of water.
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| Fig. 1 Partial 1H NMR spectra (aromatic region, 500 MHz, CD3CN, 298 K, 200 mol equivalents of D2O, total conc. = 16.6 mM) showing the dissociation of the dynamic [2]rotaxane 1a–H·PF6 with time (b = bound rotaxane and f = free components). With increasing time, the characteristic proton signals originating from the aldehyde (δ = 10.12 ppm), the free (f) pyridine ring (δ = 8.22 ppm) and the free (f) dimethoxyaryl ring (δ = 6.62 and 6.58 ppm) in separate cyclic (or acyclic) and dumbbell components were found to have their relative intensities increase while those signals arising from the rotaxane decreased. The results indicate that the dynamic [2]rotaxane dissociates slowly into its free components—2, 3a and 4–H·PF6—until the dissociation process has reached equilibrium after 24 h. With particular reference to 1a–H·PF6, there was 41% of the dynamic [2]rotaxane remaining in the mixture after 24 h. | ||
By comparing the integrations of characteristic signals arising from the dynamic rotaxanes 1a/b–H·PF6 and the dissociated free dumbbell 4–H·PF6 from the dissociation study, plots of the [Rotaxane]−1versus time can be obtained. The data, which were obtained (Fig. 2) from dissociations lasting 4–6 h, were best fitted to straight lines in agreement with second-order kinetics for both the a and b series. Rate constants (k2 and k−2), dissociation rates and half-lives (t1/2) for the breakdown of 1a/b–H·PF6 were calculated and are listed in Table 1. When comparing similar starting concentrations of the dynamic rotaxanes, in most cases, the stability to water dissociation of 1a–H·PF6 is higher than that of 1b–H·PF6. This observation may account for the enhanced template binding induced by translocational freedom involving the tetraethyleneglycol chain in 3a than that involving the more rigid 2,6-disubstituted pyridyl moiety in 3b.
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| Fig. 2 A plot of [Rotaxane]−1versus time, showing the dissociation profile of the dynamic [2]rotaxanes 1a/b–H·PF6 in the presence of different amounts of D2O. For the a series, the concentration of [2]rotaxane is 17.2, 16.6 and 15.2 mM when 100, 200 and 500 equivalents D2O were added, respectively. For the b series, the concentration of [2]rotaxane is 16.6, 15.9 and 14.9 mM when 100, 250 and 500 equivalents D2O were added, respectively. Data points were obtained from analyzing their 1H NMR spectra (500 MHz, CD3CN, 298 K). The data, which were obtained from dissociations lasting 4–6 h, were best fitted to straight lines in agreement with second-order kinetics for both the a and b series. | ||
| 1a–H·PF6 | 1b–H·PF6 | |||||
|---|---|---|---|---|---|---|
| Equivalents of water (total concentration) | 100 (17.2 mM) | 200 (16.6 mM) | 500 (15.2 mM) | 100 (16.6 mM) | 250 (15.9 mM) | 500 (14.9 mM) |
| k2/M−1 h−1 | 247.4 ± 1.2 | 355.9 ± 1.8 | 1091.2 ± 5.4 | 606.7 ± 2.9 | 1298.5 ± 6.5 | 2354.2 ± 11.7 |
| k−2/M−1 h−1 | 268.0 ± 1.3 | 247.3 ± 1.2 | 177.6 ± 0.9 | 145.0 ± 0.7 | 115.4 ± 0.6 | 82.2 ± 0.4 |
| rate/mM h−1 | 73.2 | 98.1 | 252.1 | 179.5 | 357.8 | 543.9 |
| t1/2/min | 14.1 | 10.2 | 3.6 | 5.8 | 2.8 | 1.7 |
| % Remaining [2]rotaxane in the water–acetonitrile mixture | 52 | 41 | 14 | 19 | 8 | 4 |
From a mechanistic point of view, the ring associated with the [2]rotaxanes 1a/b–H·PF6 will eventually open up (Scheme 2) with only one equivalent of H2O present in the solution to give the monoaldehyde intermediates 5a/b, allowing the dumbbell 4–H·PF6 to dethread from these intermediates on account of the loss of the crown ether's integrity and the associated pre-organisation. Subsequently, the monoaldehyde intermediates 5a/b will be hydrolysed even further right down to the diformylpyridine 2, as well as into the diamines 3a/b with one additional equivalent of H2O. However, the template effect offered by the multiple noncovalent interactions and also the stopper effect may retain the relative stability and integrity of the rotaxanes. That is, at equilibrium, relatively large amounts of H2O are required to hydrolyse the imine bond(s) and to solubilise the cleaved components.
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| Scheme 2 Plausible mechanism for the dissociation of the dynamic [2]rotaxanes 1a/b–H·PF6 into their components 2, 3a/b, 4–H·PF6, 5a/b and 6a/b. The ring associated with the [2]rotaxanes 1a/b–H·PF6 eventually opens up with only one equivalent of H2O present in the solution to give the monoaldehyde intermediates 5a/b, allowing the dumbbell 4–H·PF6 to dethread from these intermediates on account of the loss of the crown ether's integrity and the associated pre-organisation. Subsequently, the monoaldehyde intermediates 5a/b will be hydrolysed even further right down to the diformylpyridine 2, as well as into the diamines 3a/b with one additional equivalent of H2O. On the other hand, on adding one equivalent of toluidine to the [2]rotaxane solutions, dissociation occurs on account of imine exchange, which results in the fast opening of the [24]crown-8 macrocycles to give the podand-like compounds 6a/b. Toluidine plays an important role in serving as a relatively bulky imine exchange partner with the macrocycle to give a disrupted open crown (podand) that cannot be easily converted back to the [24]crown-8 derivative. | ||
Two control experiments were performed. Firstly, the dynamic [2]rotaxanes were dissolved separately in pre-dried CD3CN–DMF-d7 (9
:
1), CD3CN–CD3OD (2
:
1) and pure CD3CN. No significant changes were observed in the 1H NMR signals, from which it was concluded that dissociation of the dumbbell 4–H·PF6 does not occur even after standing for over 12 h in the presence of solvents that do not sustain hydrogen bonding. Secondly, since imine hydrolysis and formation can be catalysed by nucleophiles,8b as well as by acids,8f,16 the dissociations of the rotaxanes were investigated after adding a nucleophile—p-toluidine—as an imine exchange partner. On adding one equivalent of toluidine to the [2]rotaxane solutions, dissociation was found to occur on account of imine exchange, which results in the fast opening of the [24]crown-8 macrocycles to give the podand-like compounds 6a/b. Toluidine plays an important role in serving as a relatively bulky imine exchange partner with the macrocycle to give a disrupted open crown (podand), which cannot be easily converted back to the [24]crown-8 derivative. As a consequence, the [2]rotaxanes dissociate rapidly on simply adding one equivalent of toluidine.
The reversible formation of the [2]rotaxanes 1a/b–H·PF6 from their separate components has been demonstrated (Fig. 3) by 1H NMR spectroscopy. For example, from the dissociated mixture of the dynamic [2]rotaxane 1a/b–H·PF6 achieved on the addition of 200 equivalents of H2O (i.e., with 41% of the [2]rotaxane remaining in the mixture), after treatment with anhydrous MgSO4, the percentage of the corresponding dynamic [2]rotaxane 1a/b–H·PF6 is restored (Fig. 3a) to ∼70%. Somewhat surprisingly, molecular sieves (4 Å) are not useful for drying these systems, since the dynamic [2]rotaxanes 1a/b are unstable in their presence. Moreover, treatment with anhydrous Na2SO4, followed by evaporation and the redissolving of the dry MeCN (three consecutive cycles), gives (Fig. 3b) the corresponding dynamic [2]rotaxane 1a–H·PF6. This reversibility of the equilibrium was found to be adjustable many times over, without destroying either the individual components or the dynamic [2]rotaxanes.
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| Fig. 3 Partial 1H NMR spectra (500 MHz, CD3CN, 298 K, aromatic region) of the dissociated dynamic [2]rotaxane 1a–H·PF6 (b = bound and f = free) after treatment with (a) anhydrous MgSO4 and (b) anhydrous Na2SO4, evaporated and redissolved in MeCN through three consecutive cycles. | ||
:
1) as the eluent to yield the bisnitro compound 8 as an off-white solid (0.32 g, 30% yield); m.p. 90.2–92.4 °C. 1H NMR (500 MHz, CDCl3): δ = 3.94–3.96, (m, 4H), 4.30–4.32 (m, 4H), 4.72 (s, 4H), 7.02 (t, J = 7.7 Hz, 2H), 7.11 (d, J = 8.3 Hz, 2H), 7.38 (d, J = 7.7 Hz, 2H), 7.51 (t, J = 7.6 Hz, 2H), 7.76 (t, J = 7.7 Hz, 1H), 7.82 (d, J = 8.1 Hz, 2H); 13C NMR (126 MHz, CDCl3): δ = 68.7, 69.1, 74.1, 114.8, 120.2, 120.5, 125.5, 133.9, 137.6, 139.9, 152.1, 157.4; HRMS (HR-MALDI): calcd for C23H24N3O8m/z = 470.1563 and C23H23N3O8Na m/z = 492.1383; found m/z = 470.1560 [M + H]+ and 492.1383 [M + Na]+.Footnote |
| † Electronic supplementary information (ESI) available: NMR and mass spectra. See DOI: 10.1039/b915864b |
| This journal is © The Royal Society of Chemistry 2010 |