Kumaresh Ghosh*a,
Santanu Panjaa and
Subratanu Bhattacharyab
aDepartment of Chemistry, University of Kalyani, Kalyani-741235, India. E-mail: ghosh_k2003@yahoo.co.in; Fax: +91 3325828282; Tel: +91 3325828750 ext. 306
bDepartment of Physics, University of Kalyani, Kalyani-741235, India
First published on 19th August 2015
The gelation and anion responsive behavior of some 3-aminopyridine-based urea molecules 1–5 have been examined. Of the different pyridyl ureas, compounds 1 and 2 form an instant gel from DMSO/H2O and DMF/H2O solvents. Between the gels 1 and 2, only the gel state of 2 has been noted, for the first time, to detect iodide ions over a series of other anions through a colour change involving no phase transformation. Furthermore, the gel state of 2 is a poor semiconductor and the presence of iodide ions considerably enhances its conductivity that varies with temperature.
Inspite of reasonable progress,1a,4 the use of pyridyl ureas in the formation of anion-responsive supramolecular gels is unexplored and thus challenging.
During our ongoing work on ion recognition using chemosensors,5 we wish to shed light on anion responsive behaviour of the gel states of some simple pyridyl ureas 1–5 (Fig. 1). It is to note that the urea molecules 1,6a,b 33b and 56c are reported earlier by Steed and other groups. However, compound 2 which is the main focus of this manuscript is new and exhibits excellent anion responsive behaviour in its gel state. Of the urea molecules, 1 and 2 display excellent gelation abilities in several aqueous organic solvents. Interestingly, while the hydrogels of both 1 and 2 are thermo reversible, pH responsive and hydrogel of 2 is observed to be the good detector of iodide ion through a color change, a new observation for the first time.
Iodide recognition by artificial synthetic receptor is an important aspect in supramolecular chemistry. Iodide is an important halide linked with several biological processes such as neurological activity and thyroid function.7 In this horizon, although there are very few reports on fluorescent recognition of iodide,8 till date no report on naked eye detection of iodide using gel phase of small molecular weight supramolecular gelators is known in the literature.
In addition to pH and iodide ion responsiveness, the hydrogels of 1 and 2 are weakly semiconducting. In presence of iodide ion the conductivity of the hydrogel of 2 that varies with temperature is considerably enhanced. Low molecular-weight organic gels often possess semiconducting properties which render them unique materials for different electronic applications.9 Semiconducting properties of the gels usually arises due to self-organization of the gelators under the influence of weak forces. The tuning of these weak forces controls the spatial arrangement of individual molecular component within the aggregates. Such arrangements may establish a long-range charge delocalization within the gel matrix10 and imparts the semiconducting property. The strength of such electrical properties is influenced by the π-surface of the gelators that contribute to the stacking interaction. Addition of some dopants sometimes reinforces the semiconducting property of the gels presumably by inducing a subtle arrangement of the gelators in the gel matrix.
Close observation of the structures in Fig. 1 reveals that 3-aminopyridyl urea is connected to different aromatic and aliphatic scaffolds. Depending on the position, the pyridyl urea motif may assume different orientations. This may result in different types of hydrogen bonded networks in solution. Thus the gelation propensity of the compounds in different solvents were studied (Table 1S†). While compound 1 exhibited gelation in CH3OH/H2O and DMSO/H2O, compound 2 formed stable gel from DMSO/H2O and DMF/H2O solvent combinations. Morphologies of gels from DMSO/H2O show fibrous networks as confirmed from SEM images (Fig. 2). Structural differences between the two compounds left a significant effect on the morphology of the gels. While hydrogel of 1 is comprised of very thin, irregular, twisted fibres with a large number of void spaces to trap the solvents (Fig. 2a), compound 2 in gel state exhibits long, more regularly, closely spaced fibres to form the 3D network for solvent trapping via surface tension (Fig. 2b).
To our belief, compound 1 under the influence of hydrogen bonding of the urea groups, π-stacking of the naphthyl units and role of water in linking the pyridine ring nitrogens11 make a possible cross-linked arrangement in solution to undergo gelation (Fig. 3a). Likewise, compound 2 may follow linear packing arrangements involving the urea motifs in different ways shown in Fig. 3b and c. Instead of linear polymeric arrangement, the molecules of 2 may assume columnar packing involving similar weak non covalent forces as cited in Fig. 3b and c.
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Fig. 3 Suggested modes of interaction: (a) for 1, (b) and (c) for 2 to form the networks in solution. |
The π-stacking effect of the naphthalene motifs in 1 and 2 imparts stability to the network. Under the similar conditions, compounds 4 and 5 devoid of naphthalene groups were unable to form gel in different solvents (Table 1S†) and thereby indicated the key role of aromatic stacking. On the other hand, inspite of the presence of naphthyl unit, compound 3 (isomer of 2) did not exhibit gelation. We, therefore, presume that not only the aromatic π-stacking but also the alignment of the pyridyl ureas in forming hydrogen bonded cross-linked network in solution is crucial. It is mentionable that although compound 5 did not form gel, its copper complex as reported by Steed et al., forms colored gel.6c
A shouldering at 324 nm in UV-vis spectrum of 1 in the gel state in comparison to its sol state in DMSO:
H2O (1
:
2, v/v) is likely to be due to the formation of aggregate in the gel (Fig. 4a). In fluorescence, a weak emission at 374 nm in the sol state of 1 was significantly intensified in the gel state showing the emission at 365 nm (Fig. 4b). This fluorescence enhancement is due to aggregation formed and is in accordance with the observation reported by several groups. Similarly, in 2 the appearance of a much prominent peak at 327 nm in UV (Fig. 4c) and a broad peak at 435 nm in emission with much broadening (Fig. 4d) corroborated the formation of stronger aggregates than the case with gelator 1. In this aggregate, π-stacking interaction of the naphthalenes presumably influences to form excimer that shows emission at 435 nm. However, in both 1 and 2, the increase of fluorescence intensity for the gel states over their sol states was assigned to the phenomenon of aggregation-induced enhanced emission (AIEE).12 Upon aggregation the gelator molecules lose their mobility that results in the suppression of the nonradiative decay of the fluorophore in the gelator. In Fig. 4d, the quenching of fluorescence of the gel state of 2 containing I− ion is attributed to the heavy atom effect of I− ion.13
For better understanding the nature of emission, fluorescence decay (Fig. 2S and 3S†) and excitation spectra were measured. In time resolved emission, while the decay profile for 1 in sol state monitored at 370 nm was fitted monoexponentially, in gel state it was fitted with two components τ1 = 0.68 ns (83%) and τ2 = 2.08 ns (17%). The component 0.68 ns is attributed to the radiative lifetime of naphthalene and the component 2.08 ns is accounted for the excimer originated from the naphthalene–naphthalene stacking. In comparison, fluorescence decays for 2 in the sol and gel states monitored at 370 nm were fitted with monoexponential decay. The fluorescence decay monitored at 450 nm for gel 2 exhibited biexponential decay with the components τ1 = 1.56 ns (72%) and τ2 = 6.23 ns (28%). Table 1 represents the decay profile in details and the results indicate that the lifetime of the fluorophore naphthalene in the urea molecules 1 and 2 increases in the gel state compared to their sol states. The components originated from the aggregation also show significant increase in lifetime. The same was true for gel 2 containing KI.
Compounds (state) | λem (nm) | τ1(c) in ns | τ2(c) in ns | τav in ns | χ2 |
---|---|---|---|---|---|
1 (sol state) | 370 | 0.34(100%) | — | — | 1.11 |
1 (gel state) | 370 | 0.68(83%) | 2.08(17%) | 0.92 | 1.18 |
2 (sol state) | 370 | 0.32(100%) | — | — | 1.20 |
2 (gel state) | 370 | 1.84(100%) | — | — | 1.16 |
2 (gel state) | 450 | 1.56(72%) | 6.23(28%) | 2.86 | 1.16 |
2 with KI (gel state) | 370 | 0.70(100%) | — | — | 1.02 |
2 with KI (gel state) | 450 | 1.32(82%) | 8.14(18%) | 2.54 | 1.12 |
The excitation spectra of both the gels of 1 and 2 did not correspond in shape or position to their absorption spectra (Fig. 4S–6S†). These differences provided evidence for the ‘trapping’ or localization of excitation in the aggregate.14 The excitation spectra of 1 and 2 in the sol states also did not superimposable with their respective absorption spectra and the spectral appearance were similar to that of the cases noted in gel states. These findings indicate that in solution there is no single species in the ground state. Instead some aggregated forms coexist with the sole species.
To realize the role of urea functional groups in non covalent interaction to establish the network for gelation, we recorded the FTIR spectra of the compounds 1 and 2 in their amorphous and gel states. Comparison of the FTIR spectra for the amorphous and gel states of both 1 and 2 reveals that urea carbonyl stretching frequency in each case moves to the lower region by 4 cm−1 unit (Fig. 5). This undoubtedly indicates the involvement of the urea groups in hydrogen bonding to establish a cross linked network in the solution.
Both gels of 1 and 2 derived from DMSO/H2O showed sharp Tg. A plot of Tg vs. w/v clearly reveals that the higher the gelator concentrations greater are the stabilities of the gels (Fig. 6a). Thermal stability of hydrogel of 2 is relatively greater than the hydrogel of 1. The viscoelastic behaviour of the gel of 2 was characterised by rheological measurements, in which the storage modulus G′ and the loss modulus G′′ were measured as a functions of strain and frequency. As shown in Fig. 6b, the G′ was around four times greater than G′′, which indicated the dominant elastic character of the hydrogel exhibiting the clear thixotropic property.15
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Fig. 6 (a) Variation of gel melting temperature (Tg) with increasing concentration of gelators; (b) rheological data for DMSO![]() ![]() ![]() ![]() |
Hydrogels of both 1 and 2 were observed to be pH responsive. While in strong acidic environment the gels are broken, they started to appear when the pH of the medium lies in the range 5 to 6 for 2 and 6 to 7 for 1 (Fig. 8S†).
Since anions are known to compete with the urea hydrogen bonds,16 we were keen to know whether anions can induce the breaking of hydrogen bonds and π-stack assisted assemblies of both 1 and 2. Interestingly, while the gel of 1 from DMSO/H2O was insensitive to anions (Fig. 9S†), under identical condition the gel state of 2 was responsive selectively to iodide ion. In presence of iodide ions (counter cations: tetrabutylammonium, potassium and sodium; Fig. 10S†), the gel state of 2 exhibited sharp reddish brown coloration with time showing no phase transformation and distinguished it from other anions examined (Fig. 7). A similar observation was noticed when the DMF/H2O gel of 2 was undertaken in the study. However, the color intensity of the gel was dependent on the amount of the gelators (Fig. 11S†) as well as the concentration of KI (Fig. 8) taken in the study. It was observed that iodide ion of ∼10−2 M was much efficient in bringing intense color of the gel. This iodide-induced colored gel remained unchanged for more than three months.
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Fig. 8 Photograph showing the color changes in the DMSO![]() ![]() ![]() ![]() |
A linear increase in Tg with the added amount of KI in Fig. 9a further depicts the I− ion dependence stability of the gel. SEM images of the gel of 2 either in presence of KI (Fig. 12S†) or in presence of TBAI (Fig. 9b) reveal the more fibrous network than the gel with no I− ion. As reason, we strongly believe that the cooperative hydrogen bonding interactions of the pyridyl ureas in 2 with iodide ion or pyridine ring nitrogen bonded water–iodide supramolecular interaction17 pack the gelators of 2 efficiently due to which the stacking interaction among the naphthalene units is reinforced. In this context, in presence of I−, the broadening of the emission at 436 nm of 2 with significant quenching (Fig. 4d) supports more aggregation of the gelators compared to the gel state of 2 containing no I− ions. This is in contrast to 1 which contains one pyridyl urea. Iodide binding-induced close packing of gelators of 2 possibly influences the charge transfer interaction that results in color formation in the gel state. In the event, the possibility of formation of I3− ions (in situ generation either through oxidation of I− in presence of DMSO18a or photooxidation of I− in the gel phase) and its involvement in charge transfer complex formation cannot be ruled out. To gain insight into this fact, we recorded the UV-vis spectrum of the iodide-induced colored gel of 2 by dissolving in DMSO (Fig. 10). A band at 370 nm in the spectrum probably intimates the presence of I3− ions18b that coexist with I− ions in the gel network.
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Fig. 9 (a) Variation of gel melting temperature (Tg) of DMSO![]() ![]() ![]() ![]() |
Interestingly, when this colored gel was impregnated with aqueous solution of AgNO3 (c = 0.5 M) and was kept for longer time (∼16 h) the intensity of reddish brown colour was slowly reduced due to loss of I−/I3− ions as Ag-complexes from the gel medium (Fig. 11).
The iodide-induced color change of the gel state was also noticed in the presence of other halides. In the study, an almost colorless gel of 2 from DMSO/H2O exhibited a faint brown color in the presence of 100 μL of each solution of KF, KCl and KBr (c = 0.2 M). But addition of 500 μL of KI (c = 0.2 M) solution to this medium brought about reddish brown coloration. This suggested the negligible interference of other halides in the sensing process (Fig. 11b). This was also true in case of DMF/H2O gel of 2 (Fig. 13S†).
It is further to be pointed out that I−-induced colored gel of 2 loses its color on heating. On cooling, the transparent, colorless sol was slowly transformed into gel with its original reddish brown coloration (Fig. 12). This observation underlines the fact that I−/I3− chelation-based arrangements of molecules of 2 are presumably destroyed on heating and charge transfer no longer exists in the sol state. But on cooling, the original arrangement of molecules is set up due to which charge transfer-induced coloration is further noticed in the gel state.
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Fig. 12 Photograph showing the change in colour of the KI containing gel of 2 in DMSO![]() ![]() ![]() ![]() |
The iodide specific interaction of 2 in solution was realized from greater quenching in emission of 2 in the presence of tetrabutyl ammonium iodide (TBAI) in DMSO:
H2O (1
:
2, v/v) (Fig. 13a). Other anions showed weak interaction (Fig. 13b). However, small change in emission of 1 upon adding iodide ions suggested its weak interaction in solution (Fig. 14S†). UV-vis titration of the solution of 2 with TBAI did not produce any color of the solution and also any charge transfer band in the spectra (Fig. 15S and 16S†). Even the absence of peak in between 340 nm to 370 nm during titration indicated the mere existence of I3− in solution. This is in contrast to the findings in the gel state (Fig. 10). These observations enable us to conclude that I−/I3−-induced charge transfer only exist in the gel state.
The Benesi–Hildebrand plot19 of the change in emission intensity of 2 against the reciprocal of the TBAI concentration gave a linear fit, characteristic of 1:
1 complexation from which the association constant was estimated as 5.34 × 102 M−1 (Fig. 17S†). 1H NMR spectrum of 2 in the presence of equiv. amount of TBAI in d6-DMSO/D2O mixture solvent was observed to be negligibly perturbed and thereby suggested very weak or almost no interaction of I− into the urea binding site. In this context, it is thus believed that in fluorescence, I− ion-induced quenching of emission of 2 in solution phase is maximally due to heavy atom effect13 rather than strong hydrogen bonding interaction.
In order to gain insight into the current conductivity of the gels, we measured the current (I)–voltage (V) characteristics of the gels of 1 and 2 at room temperature (Fig. 14a). A nonlinear increase in current with increase in voltage within the measured voltage range indicated the ideal semiconducting nature of each gel. This semiconducting nature of the gels may be attributed to the π–π stacking interaction of the naphthalene units within the gel matrix which was confirmed by comparison of the UV-visible and emission spectra of 1 and 2 in their sol and gel states. Possibly due to the greater π-stacking interaction of the naphthalenes in the gel state, the gel state of 2 with much fibrous character shows better semiconducting properties than the gel of 1. It is to note that the observed semiconducting property of the gel state of 2 is almost independent of solvent. Interestingly, the gel state of 2 containing KI shows more than ten order increase in current at a particular voltage with respect to that of the normal gel. Such increase in current in presence of KI may be ascribed to the formation of I− ion binding induced charge transfer complex in the gel matrix. This is similar to the report on the semiconducting property of the perylene–iodine charge transfer complex observed by Uchida et al.20 The temperature dependency of the electrical behavior of the gel state of 2 in presence of KI shows thermally activated semiconducting nature (Fig. 14b). This semiconducting behavior persists upto temperature close to Tg of the gel above which rapid fall in current is observed. This occurs seemingly due to the disruption of the charge transfer complex that exists in the gel state.
Footnote |
† Electronic supplementary information (ESI) available: Experimental details and spectroscopic data, gelation profile, SEM image and different plots, pH responsive behaviour, anion responsive nature of 1, interference study, binding constant determination, fluorescence spectra for 1 and 2. See DOI: 10.1039/c5ra11721f |
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