Xiaojun Gua,
Binglian Bai*a,
Haitao Wangb and
Min Li*b
aKey Laboratory of Coherent Light and Atomic and Molecular Spectroscopy of Ministry of Education, College of Physics, Jilin University, Changchun 130012, PR China
bKey Laboratory for Automobile Materials (JLU), Ministry of Education, College of Materials Science and Engineering, Jilin University, Changchun 130012, PR China. E-mail: weijue@jlu.edu.cn; minli@mail.jlu.edu.cn; Tel: +86-431-85168254
First published on 23rd December 2016
The behaviors of organogels of gelators containing hydrazide and azobenzene units connected via different flexible central spacers, 1-[4-(4′-methoxylphenylazo)phenoxy]-n-[(N-(4-nitrobenzoyl)-N′-(benzoyl-4′-oxy)hydrazine)]alkane (En, n = 5, 6, 10) have been studied. The length and parity of the central flexible spacer play crucial roles in the gelation. E6 and E10 could form a stable organogel in DMF, and the critical gelation concentration of E10 is higher than that of E6, but no gelation is observed for compound E5. Xerogels of E6 and E10 from DMF exhibited fibrous aggregates. The organogels showed a photoinduced gel-to-precipitate transition under the irradiation by UV light irradiation, which was attributed to the photoisomerization of azobenzene. The trans–cis isomerization in gels further caused the morphological change from fibrous to globular aggregates. In addition, the organogel exhibited multiple stimuli-responsive behaviors upon exposure to stimuli such as temperature, anions and pH.
Supramolecular organogels and liquid crystals are fascinating organized self-assembled soft materials.14 Liquid crystal dimers are composed of molecules containing two conventional mesogenic groups linked via a flexible spacer. These materials show quite different behavior to conventional low molar mass liquid crystals and in particular their transitional behavior exhibits a dramatic dependence on the length and parity of the flexible spacer.15 We have reported that the unusual mesophase of liquid crystal dimer En (Scheme 1),16 E6 and E10 exhibit enantiotropic SmA phase, while E5 is non-mesomorphic. In addition, the melting point of E5 is much lower than that of E6, which indicated the characteristic odd–even effect in En. Recently, we reported that the effect of flexible central spacer on the trans–cis photoisomerization of azobenzene organogels.17 However, to date, there is no report of the length and parity of the central flexible spacer effect on the properties of organogels.
Our present paper focused on the gelation behavior, photo-responsive, anion-responsive and pH-responsive behavior of En (Scheme 1). The results of these studies contribute to further understanding the structure–property relationships of LMOGs.
1H-NMR spectra were recorded with a Bruker Avance 500 MHz spectrometer and Mercury-300BB 300 MHz spectrometer using dimethyl sulfoxide-d as a solvent and tetramethylsilane (TMS) as an internal standard (δ = 0.00). UV-vis absorption spectra were recorded on a Shimadzu UV-2550 spectrometer.
Spectrophotometric titrations were performed on solutions of receptors in DMF at room temperature. Anions (F−, Cl−, Br−, I− and AcO−) and NaOH were used in solution by adding the relative alkylammonium salts.
The aggregation morphologies of En were investigated by scanning electron microscopy (SEM). As shown in Fig. 1, the E6 and E10 xerogel showed 3D network, in which rigid (E6) and flexible (E10) fibers with the width of 0.5–2 μm were observed, while the concentrated solution of E5 consists of flat ribbons 2.7–3.0 μm wide (Fig. S3†). The formation of fibers or ribbons indicates that the self-assembly is driven by strong directional intermolecular interactions.
The rheological properties of the E6 and E10 gel were shown in Fig. S4.† The frequency sweep experiment (Fig. S4b and d†) of the gel reveals that G′ > G′′ and is independent of the frequency in a wide frequency region, indicating the gel nature of the sample. Stress sweep experiments (Fig. S4a and c†) of the gel indicate that the G′ and G′′ cross each other at an oscillator stress of 10 Pa, indicating the breaking of the gel to a sol state.
As shown in Fig. 2, FTIR spectroscopy of the E6 xerogel from DMF showed hydrogen-bonded N–H stretching vibrations at around 3280 cm−1, free CO at around 1701 and hydrogen-bonded CO at around 1654 cm−1, indicating that the N–H groups were mostly associated with CO groups via N–H⋯OC hydrogen bonding in the xerogel.18
In order to get more structural information, the xerogels were subjected to powder X-ray diffraction. As shown in Fig. 3, the XRD pattern of the E6 DMF xerogel exhibited sharp peaks in the lower-angle region with the d-spacings of 35.3 nm, 17.9 nm and 11.6 nm, respectively, illustrating that a lamellar organization with the interlayer distance of 3.53 nm in the gel phase, which is slightly shorter than the calculated molecular length (l = 3.68 nm) of the most extended conformation, while it is same as that of SmA1 mesophase of E6.16 In the large angle range, a peak around 2θ = 25.1° (0.35 nm) is characteristic of a typical π–π stacking distance.17,19
Fig. 4 Photographs of the DMF gel of E6 (8.0 mg mL−1) before (a) and after (b) UV light irradiation for 9 h. |
The UV light irradiation also caused the morphology change of the E6 gel. Compared to the fibrous aggregates of the xerogel in DMF (Fig. 1a), SEM image of the precipitates after UV light irradiation showed some fibers adhered some globular aggregates with diameters of 1–2 μm (Fig. 5a), whereas the cast film of the solution (developed from the gel in DMF under the UV light irradiation) showed globular aggregates, no fibers (Fig. 5b). The SEM image of the cast film of the solution after visible light irradiation on the basis of UV irradiation exhibited some globular aggregates adhered with each other (Fig. 5c).
This phase transition can be further confirmed by monitoring the UV-vis spectroscopy evolution of E6 solution in DMF (1 × 10−3 mol L−1). The UV-vis spectroscopy (Fig. 6a) showed the typical change, the intensity of the π–π* absorption peak of the trans-azobenzene moieties at 358 nm decreased with the UV light irradiation time, while that of the n–π* absorption peak of the cis-azobenzene at 448.5 nm increased concomitantly, indicating that photoinduced trans–cis isomerization took place and eventually brought about the gel–precipitate transition. Fig. S9† showed the reversibility in the photoisomerization by alternate irradiation of UV and visible light. The conversion efficiency of cis-azobenzene reached ca. 87% at the photo-stationary state within 18 s, estimated from the UV-vis absorption spectra (Fig. 6a), whereas the trans-azobenzene only can be recovered ca. 51% at the photo-stationary state within 9 s (Fig. 6b). The trans-azobenzene cannot be all recovered was also confirmed by the 1H-NMR under irradiation by 450 nm visible light (Fig. S10c†), but the trans-azobenzene can be recovered by heating (Fig. S10d†) or place in darkness enough time after UV or visible light irradiation (Fig. S11†).
Fig. 6 UV-vis spectra of E6 solution in DMF (1 × 10−3 mol L−1) (a) under UV light irradiation for 0–18 s; (b) under visible light irradiation for 0–9 s. |
The FTIR spectrum of E6 in the precipitate (developed from the DMF gel under the UV irradiation) (Fig. 7a) showed characteristic bands of N–H stretching modes of amide groups at 3240 cm−1, which is 40 cm−1 shorter than that in the gel state. In addition, the CO stretching vibration shifted from 1701 cm−1 and 1654 cm−1 (gel state) to 1654 cm−1 (precipitate). It is obviously that the intermolecular hydrogen bonding between N–H and CO in the precipitate was stronger than that in gel state (Fig. 7b).
Fig. 7 FTIR spectra of (a) xerogel of E6 in DMF; (b) the precipitate developed from the gel in DMF under the irradiation of 365 nm UV light for 9 h. |
Combining the above results, we proposed a possible mechanism of photoinduced gel–precipitation change. E6 molecules in the gel state are dominantly in the trans-conformation, which self-assembled to layered aggregation to form the stable gel, and the main driving forces for gelation were intermolecular hydrogen bonding between the hydrazide groups and π–π interactions between the azobenzene groups. Meanwhile there exists the equilibrium among the assembled fibrous network and the dissolved small assemblies and the molecularly dispersed trans-En. Irradiation of the gel by UV light firstly leads to trans–cis isomerization of the azobenzene units in the dissolved assemblies and the molecularly dispersed trans-En. In the cis-isomers the dipole moment value increases, which improves the solubility of the E6 in DMF (polar solvent). With the increase of irradiation time, a certain amount of trans-isomers in fiber of organogel also turns into cis-isomers and then dissolves, thus the concentration of cis-isomers increases and further globular aggregates form. Meanwhile, the rest of fiber of trans-isomers in original organogel cannot support the large volume of organic liquid, so results in the organogel disintegrating and some fiber of trans-isomers precipitated out simultaneously.
Fig. 8 Photograph of E6 organogels (8 mg mL−1) upon adding of 10 equiv. of various anions in DMF, from left to right: none, F−, AcO−, Cl−, Br−, I−. |
Fig. 9 UV-vis spectra of E6 (1 × 10−4 mol L−1) in DMF upon addition of 10 equiv. of various anions (F−, Cl−, Br−, I−, AcO−). |
The evidence for the anion-responsive mechanism was obtained from 1H NMR experiments in DMSO-d6 in Fig. S17,† the addition of 5 equiv. F− resulted in the disappearance of the signals at 10.46 ppm and 10.64 ppm of the NH protons, and the appearance of a weak signal at δ = 10.44 ppm, indicating the formation of N–H⋯F− hydrogen bond, simultaneously, a new weak signal appeared at δ = 15.71 ppm, which implied the formation of a stable bifluoride hydrogen-bonding self complex (HF2−)20–22 and the occurrence of bifluoride points to the deprotonation of either the N–H group. After addition of 3 equiv. of AcO− ions, the NH signal disappeared, suggesting that only a hydrogen-bond complex [En·AcO]− is observed in Fig. S18.†
In addition, the gel–gel colorimetrical sensor can be obtained through two-component organogel based on E5 and 4-poxd-B8 gelator in the Fig. 10 (the molar ratio 1:1, the molecular structure of 4-poxd-B8 was shown in Fig. S19†23,24). As shown in Fig. S20, S21, S23 and S24,† the UV-vis and 1H NMR spectra indicate that there is no interaction between the 4-poxd-B8 and E5, as well as the 4-poxd-B8 and F−. The presence of F− can not disrupt the preformed gel into a solution through slow diffusion of the F−, only can change the color of the two-component organogel (Fig. 10). The F− only can interact with E5, the role of the 4-poxd-B8 is to form 3D cross-linking network by self-assembling to support the solvent to form organogel and keep the organogel without disassembly in the presence of F−, which is in agreement with the morphology as shown in Fig. S22.†
Fig. 10 Reversible gel–gel color transition of the two-components gel of 4-poxd-B8 and E5 (the molar ratio 1:1) in DMSO triggered by F− and AcO−. |
Fig. 11 UV-vis absorption spectra of E6 in the presence of (a) NaOH (0–18 equiv.); (b) HCl in DMF (1 × 10−4 mol L−1). |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c6ra24886a |
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