Deepta
Chattapadhyay
,
Sujay Kumar
Nandi
and
Debasish
Haldar
*
Department of Chemical Sciences, Indian Institute of Science Education and Research Kolkata, Mohanpur-741246, West Bengal, India. E-mail: deba_h76@yahoo.com; deba_h76@iiserkol.ac.in
First published on 11th January 2022
The effect of isomerism on the structure, self-assembly and properties of two peptide mimetics has been investigated. These peptide mimetics contain m-aminobenzoic acid, p-aminobenzoic acid and N,N′-dicyclohexylurea. From X-ray crystallography, it is observed that the p-isomer adopted a kink-like conformation stabilized by C–H⋯π interactions and formed a supramolecular anti-parallel duplex and layer by layer sheet-like structure in higher order assembly. However, only the m-isomer formed sonication responsive gels in different hydrocarbons such as hexane–EtOAc (19:1), diesel, kerosene, body oil and coconut oil. From rheology experiments, the gel was found to have physical cross-links and is elastic in nature. The FE-SEM images depicted that the m-isomer exhibited nanofiber network morphology, whereas the p-isomer exhibited polydisperse microsphere morphology. The gel was found to be highly sensitive to alcohol vapours, although the kinetics become much slower from methanol to ethanol to isopropanol. The gel is also very responsive to acid vapours like HCl.
Stimuli responsive materials have attracted huge attention due to their selective sensing ability. The inherent properties (volume, color, or viscosity) of these materials change by sensing an analyte.8 Among different stimuli responsive materials, the ones whose fluorescence output can be tuned by external stimuli like pH, ions, light, temperature, redox potential, and vapours are highly promising.9 These luminescent materials are already being used in sensing devices, memory and display devices, for the fabrication of detectors and in thermal imaging.10–12 In this context, the development of a VOC responsive self-assembled smart material will be very useful. Self-assembly is generally driven by various secondary interactions such as hydrogen bonding, π–π stacking, C–H⋯π interactions, dipole–dipole interactions, and van der Waals interactions. Earlier, different groups have reported VOC sensors based on cavitands,13,14 metal–organic frameworks,15,16 luminescent materials,17,18 and organic vapochromic materials.19,20
Previously we have reported an on-line ammonia sensor and invisible security ink using a fluorescent zwitterionic spirocyclic Meisenheimer complex.21 We have also shown that a self-healing hydrogel from a dipeptide can act as a HCl sensor.22 Recently, we have reported a robust tripeptide for in-field selective naked eye ultratrace detection of 2,4,6-trinitrophenol.23 Herein, we have reported the effect of isomerism on the structure, self-assembly and properties of two peptide mimetics. From X-ray crystallography, it is observed that the p-isomer adopted a kink-like conformation stabilized by C–H⋯π interactions and formed a supramolecular anti-parallel duplex and layer by layer sheet-like structure in higher order assembly. Interestingly, the m-isomer formed sonication induced organogels in different hydrocarbons such as hexane–EtOAc (19:1), diesel, kerosene, body oil and coconut oil. From rheology experiments, the gel is found to have physical cross-links and to be elastic in nature. FE-SEM images depicted that the m-isomer exhibited nanofiber network morphology, whereas the p-isomer exhibited polydisperse microsphere morphology. The gel was found to be highly sensitive to alcohols. However, the kinetics become much slower from methanol to ethanol to isopropanol. The gel is also very responsive to acid vapors like HCl.
The final compounds have been purified by column chromatography and characterized by 1H-NMR, 13C-NMR, FT-IR and mass spectrometry analysis. Peptide mimetic 2 was also characterized by single crystal X-ray diffraction analysis. We have failed to develop crystals of peptide 1 suitable for X-ray crystallography. Peptide mimetic 2 crystallizes with one molecule in the asymmetric unit from methanol–water solution by slow evaporation (Fig. 1a). The compound adopted a kink like structure and is stabilized by C–H⋯π interactions (Fig. 1a). The C–H to centroid distance is 3.9 Å. There is no intramolecular hydrogen bond. Moreover, the peptide mimetic 2 self-assembles through reciprocal intermolecular hydrogen bonds (N4–H4⋯O1, 2.14 Å, 2.978 Å, 166°, 1 − x, 1 − y, 1 − z) to form an anti-parallel duplex structure (Fig. 1b). The duplex is also stabilized by intermolecular C–H⋯π interactions (Fig. 1c). The packing diagram of peptide mimetic 2 shows that the dimers further self-assemble to form a supramolecular 1D structure through intermolecular hydrogen bonds (N5–HA⋯O2, 2.32 Å, 3.123 Å, 156°, 1 − x, 1 − y, 2 − z and N5–HB⋯O2, 2.4 Å, 3.018 Å, 129°, −1 + x, y, z) along the crystallographic a axis (Fig. 1d).
In higher order packing, peptide mimetic 2 forms a layer by layer sheet-like structure (Fig. 2) along crystallographic a and b directions. Though there is no π–π stacking interaction, the aromatic rings formed one layer which is sandwiched between two hydrophobic cyclohexane layers (Fig. 2).
Initially, the gelation abilities of the peptides were investigated in various organic solvents by dissolving 10 mg of compound in 1 mL of solvent followed by the heating–cooling technique. But the compounds did not form gels (ESI,† Fig. S2). But on sonication for 20 minutes, we observed that peptide mimetic 1 formed organogels in hexane. However, on addition of 5% (v/v) ethyl acetate, the sonication-induced gelation occurred instantly (Fig. 3a). The gel formation was confirmed by an inverted vial test. Peptide mimetic 1 also formed gels in different oils such as diesel, kerosene, body oil and coconut oil after sonicating for 1–2 minutes (Fig. 3). The gels are opaque in nature. The minimum gelation concentration (MGC) for peptide mimetic 1 was found to be 5 mg mL−1. The peptide mimetic-based sonication responsive gel showed high stability for a couple of weeks. Similar conditions were tried for the p-isomer 2, but it failed to show any gelation behaviour in different organic solvents even at high concentrations.
Rheology experiments were performed to measure the mechanical strength of the organogel. Rheology data were taken as a function of angular frequency and oscillatory strain (Fig. 4). In rheology, there are two main parameters, the elastic response which is measured using storage modulus G′ and the viscous response which is measured using loss modulus G′′. In the frequency sweep experiment, the storage modulus G′ is one order of magnitude higher than the loss modulus G′′ over the entire angular frequency range, which confirms the formation of the elastic gel by physical cross-linking through weak interactions (Fig. 4a). In the amplitude sweep experiment, the loss modulus G′′ becomes greater than storage modulus G′ at 1.1% oscillation strain, which indicates that the gel breaks after this strain (Fig. 4b).
Fig. 4 Rheology of organogels of peptide mimetic 1 in 19:1 hexane/ethyl acetate, (a) frequency sweep experiment and (b) oscillation strain. |
Peptide mimetic 1 gels exhibit amazing self-healing26 properties. When we placed two pieces of a gel together, one in body oil and the other in kerosene oil, we observed, to our surprise, that the two oils slowly got mixed together. Within 12 hours, two gel bars formed a single bar and the oils were completely mixed with each other indicating the self-healing nature of the gel (ESI,† Fig. S3). The self-healing may be due to the dynamic equilibrium between the generation of the new fibers and the disconnection of the old fibers and that governs the reformation of the gel. But the organogel is not thixotropic.
The morphologies of the peptide mimetic 1 gels were examined using a polarized optical microscope (POM). The xerogels of the organogel formed in the hexane/EtOAc mixture show a micro-fibre like morphology under a polarized optical microscope (ESI,† Fig. S4a). The morphology of peptide mimetic 2 was also investigated. For that, a drop of the peptide mimetic 2 solution in hexane was placed on a microscopic glass slide and allowed to dry at room temperature for one day. It was observed that peptide mimetic 2 forms microsphere like morphology (ESI,† Fig. S4b). To better understand the morphologies of the gels, field emission scanning electron microscopy (FE-SEM) is a wonderful technique. From FE-SEM, xerogels of peptide mimetic 1 obtained from hexane/EtOAc show the branch of nanofibers of length up to few micrometers (Fig. 5a and b). The average diameter of the fibers is 25 nm. The nanofibers are interlinked to produce a 3D network that can entrap solvents (Fig. 5b). From FE-SEM images, it was observed that peptide mimetic 2 forms polydisperse microsphere like morphology (Fig. 5c and d). The average diameter of the microspheres is 300 nm.
Fig. 5 (a and b) FE-SEM images of the xerogels of peptide 1 from hexane/EtOAc showing nanofiber network morphology. (c and d) FE-SEM images of peptide 2 showing polydisperse microsphere morphology. |
Only peptide mimetic 1 forms an organogel, which indicates that the H-bonding through the aromatic amine group might play a crucial role in gelation. This fact is further supported by the observation that on addition of a polar protic solvent, the gel breaks. FT-IR spectroscopy is a very useful technique to probe this, since H-bonded amine gives a different signal from that of a free amine. The FT-IR spectra of the as-synthesized peptide mimetic 1 in the KBr pellet show three peaks due to NH stretching. The two peaks at 3298 cm−1 and 3348 cm−1 correspond to the aromatic amine stretching whereas the peak at 3438 cm−1 corresponds to the non-hydrogen bonded amide NH stretching (Fig. 6). The IR spectra of xerogels show a broad signal with a peak at around 3341 cm−1 indicating the presence of hydrogen bonded NH. This supports the role of H-bonding in sonication-induced gelation of peptide mimetic 1. The two separate carbonyl peaks at 1682 cm−1 and 1634 cm−1 for peptide mimetic 1 also get broadened and appear as one peak at around 1630 cm−1 for the xerogel (Fig. 6). The peptide mimetic 2 shows NH stretching at 3369 cm−1 and 3312 cm−1 corresponding to the hydrogen bonded NH and amide I and amide II at 1680 cm−1 and 1540 cm−1.
Moreover, the peptide mimetic 1 organogel can be used as a sensor for volatile acids. This is very interesting for pollutant detection, the automotive industry and the chemical industry. HCl vapor was charged to the organogel of peptide mimetic 1; on contact with HCl the gel transforms to a sol (Fig. 7). In the presence of HCl, the amine functional group of the gelator gets protonated and the gel transforms to sol. The gel also breaks on addition of acids such as H2SO4 and HNO3 (ESI,† Fig. S5). The gel is sensitive to acetic acid but not to formic acid, ammonia, methyl amine and ethyl amine (ESI,† Fig. S5). The process of acid vapour sensing using the peptide mimetic 1 organogel can be upgraded to an on-line process for safety related application in industries which use or produce large amounts of concentrated acids.21
Fig. 7 (a–c) Sensitivity of the peptide mimetic 1 organogel towards HCl gas. (d) Sensitivity of the peptide mimetic 1 organogel towards alcohols. |
It is interesting to note that the organogel of the peptide mimetic 1 was found to be highly sensitive towards alcohols. Even, the gel broke immediately after addition of as little as 10 μL of MeOH. However, it was not specific to methanol only; ethanol and isopropanol could also break the gel (Fig. 7d). The kinetics become much slower as we go from methanol to ethanol to isopropanol. However, the gel remains intact when other organic solvents such as DCM and acetone are added.
Footnote |
† Electronic supplementary information (ESI) available: Peptide synthesis, NMR spectroscopy, Fig. ESI S1–S16, and peptide single crystals. CCDC 2006754. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/d1ma00992c |
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