Arpita Paikar,
Apurba Pramanik and
Debasish Haldar*
Department of Chemical Sciences, Indian Institute of Science Education and Research Kolkata, Mohanpur, West Bengal 741246, India. E-mail: deba_h76@yahoo.com; deba_h76@iiserkol.ac.in; Fax: +91 3325873020; Tel: +91 3325873119
First published on 27th March 2015
Different assembly and behaviour of homologous discotic tricarboxyamides containing β-alanine and γ-aminobutyric acid have been investigated. From UV/Vis and FT-IR spectroscopy the tricarboxyamides have similar self-assembly patterns. But, the tricarboxyamide 2 containing γ-aminobutyric acid residues forms a gel in aromatic solvents after heating, cooling and ageing. However, the β-alanine analogue 1 failed to form a gel under the same conditions. From FE-SEM studies the tricarboxyamide 1 shows unbranched rod like morphology but the tricarboxyamide 2 exhibits an entangled fiber network. Finally, the X-ray crystallography reveals that both the tricarboxyamides 1 and 2 adopt 3-fold intermolecular H-bonded helical columnar structures. Detailed structural analysis shows that the individual helical columnar structures of tricarboxyamide 2 are themselves self-assembled through multiple hydrophobic interactions between side chains and thereby form a supramolecular network structure. However, the tricarboxyamide 1 columns are self-assembled into a supramolecular bundle-like structure. The result indicates that side chain interactions have a drastic effect on quaternary structure and function.
Intrigued by the previous knowledge, we wanted to investigate the assembly of discotic tricarboxyamides with flexible hydrophobic side chains. Herein we present influence of side chain interactions on quaternary structure and function of tricarboxyamides. The tricarboxyamides 1 and 2 contain 1,3,5-benzene tricarboxylic acid and β-alanine and γ-aminobutyric acid. From UV/Vis, FT-IR and NMR spectroscopic studies the tricarboxyamides 1 and 2 have same self-assembly pattern. Interestingly the tricarboxyamide 2 containing γ-aminobutyric acid residues form organogel in aromatic solvents after heating, cooling and ageing. But the β-alanine analogue 1 failed to form gel under same condition. FE-SEM images show that the tricarboxyamide 1 has unbranched rod like morphology but the tricarboxyamide 2 has entangled fibers network. Single crystal X-ray diffraction studies exhibit that both the tricarboxyamide 1 and 2 adopts 3-fold intermolecular H-bonded helical columnar structure. In higher order, the tricarboxyamide 1 columns are self-assembled to form bundle-like structure. But, the individual helical columnar structure of tricarboxyamide 2 self-assembled through multiple hydrophobic interactions between side chains to form a supramolecular network structure.
To investigate the self-assembly behaviour of tricarboxyamide 1 and 2, a wide variety of different spectroscopic techniques have been used. The typical UV/Vis absorption spectra of tricarboxyamide 1 in methanol (0.023 mM) show an absorption band at 208 nm for π to π* transition (Fig. 1a). However, increasing the concentration of tricarboxyamide 1 induces stacking interactions between the molecules. The bathochromic shift of 17 nm of the absorption band with increasing concentration indicates J-type aggregation of tricarboxyamide 1.29 The absorption spectra of tricarboxyamide 2 in methanol also show an absorption band at 208 nm and bathochromic shift of 17 nm with increasing concentration (Fig. 1b). These results show that the tricarboxyamides 1 and 2 have similar aggregation pattern.
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| Fig. 1 Concentration dependent UV/Vis spectra of (a) tricarboxyamide 1 and (b) tricarboxyamide 2 showing J-type aggregation in methanol. | ||
Solid state FT-IR spectroscopy is an excellent method to investigate the self-assembly propensity of the reported tricarboxyamides. In FT-IR, the region of 3500–3200 cm−1 is important for the N–H stretching vibrations however the range 1800–1500 cm−1 is assigned for the stretching band of amide I and the bending peak of amide II and ester groups. The FT-IR spectra of tricarboxyamide 1 (Fig. 2a) exhibits N–H stretching frequency at 3246 cm−1 for non hydrogen bonded N–H and amide peaks at 1637 and 1559 cm−1 indicating the presence of threefold intermolecular H-bonding between neighbouring molecules within the columnar structures.30 The peak around 1741 cm−1 is responsible for the non hydrogen bonded ester carbonyls. The tricarboxyamide 2 exhibits peak at 3237 cm−1 for N–H stretching frequency. The amide and methyl ester have appeared at 1742, 1636 and 1562 cm−1 (Fig. 2b). These results indicate that the tricarboxyamides 1 and 2 have similar self-assembly propensity.
But, the tricarboxyamides exhibits different gelation behavior in aromatic solvents. The gelation propensities of tricarboxyamides 1 and 2 have been studied in a wide variety of organic solvents using conventional heating-cooling techniques.31 However, the tricarboxyamides 1 did not form gel in aromatic hydrocarbon like toluene, o-xylene, m-xylene, p-xylene, 1,2-dichlorobenzene. But when solutions of the reported tricarboxyamides 2 in various organic solvents (ESI Table 1†) were subjected to heating-cooling techniques, homogeneous gelation in aromatic hydrocarbon like toluene, o-xylene, m-xylene, p-xylene was observed. The gelation has been confirmed by the inverted vial method.32 The opaque gels of tricarboxyamides 2 are stable for 2–3 months at room temperature and the gels are thermoreversible (ESI†).
The information about the type of network (tertiary structure) responsible for the observed gelation of tricarboxyamide 2 in toluene was obtained from rheology. The storage modulus (G′, a measure of the elastic response of the material) of the gel (10 wt%) was found to be larger than the loss modulus (G′′, a measure of the viscous response), indicative of an elastic rather than viscous material (Fig. 3).13 Such rheological behaviour is a characteristic of physically cross-linked gel via weak interactions.13
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| Fig. 3 Mechanical response of tricarboxyamide 2 gel in toluene at 20 °C with small oscillatory shear in the linear viscoelastic regime. | ||
Further, to investigate the self-assembly behaviour of tricarboxyamide 2 in organogel, variable temperature 1H NMR spectroscopic experiments have been performed. The experiments started with tricarboxyamide 2 gel in toluene-D8. From the stack plot, the downfield shifts of amide protons upon heating suggest that the intermolecular three fold hydrogen bonds are broken with increasing temperature. Whereas the 1,3,5-benzene tricarboxylic acid protons exhibit upfield shifts up to 85 °C (gel melting temperature) and show downfield shifts at higher temperature (Fig. 4). Moreover, α, β and γ protons of γ-amino butyric acid residues exhibit significant downfield shifts upon heating which suggest that the intermolecular hydrophobic interactions are also changed with increasing temperature. The tricarboxyamide 1 does not form gel in toluene-D8. Under same variable temperature 1H NMR spectroscopic experiments, the tricarboxyamide 1 does not exhibit any significant shift of α and β protons of β-alanine residues (ESI Fig. S1†). Hence, not only the hydrogen bonding and π–π stacking interactions but also the hydrophobic interactions plays an important role in self-assembly and gelation of tricarboxyamide 2.
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| Fig. 4 Part of the 1H NMR spectra of tricarboxyamide 2 gel in toluene-D8 with increasing temperature. | ||
The field emission scanning electron microscope (FE-SEM) has been used to study the morphology of the reported tricarboxyamide 2 xerogel obtained from various aromatic solvents. The FE-SEM micrographs of the corresponding xerogels from toluene, o-xylene, m-xylene and p-xylene exhibit the entangled networks of unbranched fibers with 1 μm average diameter and several micrometers in length (Fig. 5).
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| Fig. 5 FE-SEM images showing entangled networks of fibers of tricarboxyamide 2 xerogel from (a) toluene, (b) o-xylene, (c) m-xylene and (d) p-xylene. (Inset: the picture of the organogels). | ||
To examine the difference in morphology, we have also studied the solution of tricarboxyamides 1 or 2 in 1,2-dichloro benzene by field emission scanning electron microscope (FE-SEM). For FE-SEM, The freshly prepared solution of tricarboxyamides in 1,2-dichloro benzene (5 mg mL−1) was drop-casted onto a silicon wafer and dried by slow evaporation. The material was then allowed to dry in a vacuum at 30 °C for two days. From FE-SEM image (Fig. 6a) the tricarboxyamide 1 exhibits unbranched polydisperse crystalline morphology. The crystals are very rigid and several micrometer in length. However, FE-SEM image of the tricarboxyamide 2 shows the entangled fibers network morphology (Fig. 6b). This three dimensional network of entangled fibers (physical crosslinks) helps to entrap solvent molecules and forms organogel.33
Clear evidence of inter column interactions between side chains has confirmed by X-ray crystallography.34 Tricarboxyamide 1 crystallizes with three molecules in the asymmetric unit (ESI Fig. S2†). The ORTEP diagram (ESI Fig. S2†) of tricarboxyamide 1 shows that the amide groups in a molecule are out of the central ring plane though two amides are tilted toward the same direction and third one in opposite direction. Two β-alanine residues adopt gauche conformation and third one adopts anti conformation (Fig. 7a). The torsion angles around the central benzene core and the β-alanine residues appears to play a critical role in dictating the overall structural features of tricarboxyamide 1. Moreover, structure of 1 exhibit that the two β-alanine residues are in the same face and the third one is in the opposite face of the central benzene ring (Fig. 7a). From X-ray crystallography, it is evident that the asymmetric unit contains one molecule of tricarboxyamide 2. The ORTEP diagram (ESI Fig. S3†) of tricarboxyamide 2 shows that two γ-aminoburytic acid residues adopt gauche–gauche conformation and third one adopts gauche–anti conformation (Fig. 7b). The amide groups are out of the central ring plane. However, aromatic amides prefer coplanarity of the carbonyl functional group with the aryl system to optimize conjugation, in tricarboxyamide 2 the amides are tilted toward the same direction (Fig. 7b). This is because of the competition between the demand of conjugation (amide and aryl) and that of intermolecular NH⋯O
C hydrogen bonding. The solid state structure of 2 exhibits that the two γ-amino butyric acids are in the same face and the third one is in the opposite face of the central benzene ring (Fig. 7b).
The crystal structure further reveals that the individual tricarboxyamide 1 subunits are stacked on top of another by threefold intermolecular H-bonding interaction between neighbouring molecules and generate a supramolecular column like structure (Fig. 8a) about crystallographic c direction.35 The hydrogen bonding parameters of tricarboxyamides are listed in Table 1. The columnar arrangement also stabilized by strong π–π stacking interactions. The center-to-center distance between the benzene rings in columnar assembly is about 3.541 Å. The J-type aggregation of the tricarboxyamide 1 molecules helps to place the β-alanine residues in a regular helical manner outside of the columnar central aromatic core (Fig. 8a). Hence, the tricarboxyamide 1 column looks like a circular block on top view (Fig. 8b). The tricarboxyamide 2 also exhibits supramolecular columnar structure stabilized by 3-fold intermolecular H-bonding interactions in solid state.35 The individual discotic tricarboxyamide 2 molecules are themselves stack one top of another and regularly interlinked through intermolecular hydrogen bonding interactions (N1–H1⋯O5, N2–H2⋯O6, and N3–H3⋯O8) to form the helical columnar assembly along crystallographic b direction (Fig. 8c). There also exist a strong π–π interaction between adjacent aromatic ring. The centre-to-centre distance between the benzene rings in columnar assembly is about 3.486 Å. Outside of the columnar central aromatic core, the γ-amino butyric acid residues are hanging in linear fashion (Fig. 8c). Hence, the tricarboxyamide 2 column looks like a star on top view (Fig. 8d).
| D–H⋯A | D⋯H (Å) | H⋯A (Å) | D⋯A (Å) | D–H⋯A (°) | |
|---|---|---|---|---|---|
| a Symmetry equivalent a: 1 − x + y, 1 − x, 1/3 + z, b = 1 − y, x − y, −1/3 + z, c = x − y, x, −1/6 + z, d = y, −x + y, 1/6 + z, e = 1/2 − x, −1/2 + y, 1/2 − z. | |||||
| 1 | N1–H1⋯O12 | 0.86 | 2.08 | 2.920(6) | 165 |
| N2–H2⋯O16 | 0.86 | 2.18 | 3.021(6) | 167 | |
| N3–H3⋯O13a | 0.86 | 1.95 | 2.800(6) | 168 | |
| N4–H4⋯O3b | 0.86 | 2.09 | 2.906(7) | 158 | |
| N5–H5⋯O7 | 0.86 | 1.96 | 2.796(6) | 165 | |
| N6–H6⋯O4b | 0.86 | 2.09 | 2.945(7) | 172 | |
| N7–H7A⋯O21c | 0.86 | 2.05 | 2.869(6) | 159 | |
| N8–H8⋯O22d | 0.86 | 2.02 | 2.858(7) | 166 | |
| N9–H9⋯O25c | 0.86 | 2.11 | 2.963(6) | 171 | |
| 2 | N1–H1⋯O5e | 0.86 | 2.04 | 2.861(3) | 158 |
| N2–H2⋯O6e | 0.86 | 2.06 | 2.873(3) | 157 | |
| N3–H3⋯O8e | 0.86 | 2.02 | 2.856(3) | 165 | |
The packing diagram further reveals that the individual tricarboxyamide 1 columns are self-assembled and generate a supramolecular bundle-like framework along crystallographic a and b directions (Fig. 9). This type of packing leads to unbranched rod-like morphology for tricarboxyamide 1. From X-ray crystallography, in higher order packing, the individual helical columnar structure of tricarboxyamide 2 are themselves self-assembled through multiple hydrophobic interactions (between γ-amino butyric acid's β methylenes and between ester methyl groups), and thereby form a supramolecular structure along the crystallographic a and c direction (Fig. 10). The intermolecular C–H⋯O hydrogen bonds36 (C16–H16B⋯O7, 2.54 Å, 3.48 Å, 166°, −1 + x, y, z) also help to stabilized the supramolecular structure. For tricarboxyamide 2, the side-chains interactions (physical crosslinks) help to develop entangled fibers network morphology which entrap solvent molecules and forms organogel.
:
2 (EtOAc
:
hexane) as eluent of the crude product yielded 0.326 g of 1. Yield 31.46%.1H NMR (400 MHz, CDCl3, δ in ppm): 8.331 (s, 3H, aromatic ring proton), 7.763–7.734 (t, 3H, J = 5.8 Hz, NH), 3.649–3.633 (d, 6H, J = 6.4 Hz, CβH of β-Ala), 3.614 (s, 9H, OCH3), 2.624–2.593 (t, 6H, J = 6.2 Hz CαH of β-Ala). 13C NMR (100 MHz, CDCl3, δ in ppm): 173.172, 166.793, 134.881, 129.246, 52.292, 36.360, 33.948. Mass spectra: m/z 488.1751, [M + Na]+; M calcd 465.2.
:
2 (EtOAc
:
hexane) as eluent of the crude product yielded 0.4166 g of 2. Yield 33.27%.1H NMR (500 MHz, CDCl3, δ in ppm): 8.007 (s, 3H, aromatic ring proton), 7.842–7.821 (t, 3H, J = 5.25 Hz, NH), 3.561 (s, 9H, OCH3), 3.330–3.292 (q, 6H, J = 6.33 Hz, CγH of Gaba), 2.317–2.288 (t, 6H, J = 7.25 Hz CαH of Gaba), 1.808–1.1780 (t, 6H, J = 7 Hz CβH of Gaba). 13C NMR (100 MHz, CDCl3, δ in ppm): 173.595, 166.697, 134.920, 128.097, 51.481, 39.357, 31.175, 24.257. Mass spectra: m/z 530.1033, [M + Na]+; M calcd 507.2.
Footnote |
| † Electronic supplementary information (ESI) available: Synthesis and characterization of trisamides, 1H NMR, 13C NMR, Fig. S1–S10. CCDC 1051708 and 1011367. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c5ra03864b |
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