Sarah J.
Pike
*ab,
Richard
Telford
b and
Louise
Male
a
aSchool of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2TT, UK. E-mail: s.j.pike@bham.ac.uk
bSchool of Chemistry and Biosciences, Faculty of Life Sciences, University of Bradford, Bradford, West Yorkshire BD7 1DP, UK
First published on 11th August 2023
We report on a convenient synthetic route to rapidly access a new photo-responsive ortho-azobenzene/2,6-pyridyldicarboxamide heterofoldamer. The adoption of a stable helical conformation has been established for this scaffold in both the solid state and in solution using single crystal X-ray diffraction and circular dichroism (CD) spectroscopy respectively. Reversible control over the stimuli-driven structural re-ordering of the supramolecular scaffold, from a stable helical conformation under non-irradiative conditions, to a less well-ordered state under irradiative conditions, has been identified. The robust nature of the responsive, conformational, molecular switching behaviour has been determined using UV/Vis, 1H NMR and CD spectroscopy. Minimal loss in the efficiency of the stimuli-driven, structural re-ordering processes of the foldamer scaffold is observed, even upon multiple cyclic treatments with irradiative/non-irradiative conditions.
Foldamers are synthetic helical oligomers that adopt stable secondary structures in solution.3 In recent years, there has been a significant drive to create stimuli-responsive foldamers that have the ability to, in part, replicate the conformational switching behaviour demonstrated by complex natural systems. Stimuli-responsive foldamers have attracted growing interest due their widespread applications in a number of fields including synthesis, as organocatalysis4 and supramolecular chemistry, as sensors and probes,5 receptors6,7 and for signalling applications.8 The emergent biological properties of foldamers as potential antibiotics has also garnered significant attention.9
Photo-responsive foldamers are attractive scaffolds as they offer a reliable and reversible method by which to control the conformational preferences of these supramolecular systems.10–18 Generally, photo-responsive foldamers are able to demonstrate controlled molecular switching between a stable helical conformation to a random coil or less well-folded state, in the presence and absence of light, respectively.10,11 To achieve photo-driven conformational molecular switching in these supramolecular scaffolds, photo-responsive units (e.g. azobenzene or spiropyran) are incorporated at the side-chain14–16 or in the backbone17,18 of the oligomer. Foldamers based on the latter design strategy are often able to demonstrate higher levels of control over the conformational switching behaviour of the scaffold due to their importance in maintaining the integrity of the global folded structure.19
Many photo-responsive foldamers are created using the heterofoldamer design approach, wherein, the foldamer scaffold is composed of two or more distinct monomer building blocks.16–20 The implementation of this design approach is highly attractive as it offers a convenient method by which structural diversity can be directly incorporated into the scaffold. In 2006, Parquette and co-workers elegantly exploited the heterofoldamer design approach to create a class of photo-responsive foldamers that incorporated alternating sequences of pyridine-2,6-dicarboxamide and meta-(phenylazo)azobenzene units within the oligomer backbone.18a However, despite recent advances in the development of photo-responsive foldamers, existing routes to access these supramolecular systems can be synthetically demanding, for example, in Parquette's original scaffold 12 steps are required to access a two-turn foldamer.18a,21 Additionally, information about the robustness of the light-driven molecular switching behavior of photo-responsive foldamers can also be limited. These drawbacks can both restrict the accessibility of these supramolecular scaffolds and hinder our understanding of their operational practices, which in turn, can limit our ability to optimize the future design of these responsive systems.
Herein, we outline on the development of a short five-step synthetic route to rapidly access a photo-responsive heterofoldamer based on an alternating ortho-azobenzene/2,6-pyridyldicarboxamide motif. The light-responsive heterofoldamer described in this work is related to Parquette's original scaffold18a but the simplified design approach reported, herein, enables a significantly more streamlined synthetic route to be adopted, thus, considerably increasing its synthetic accessibility. The controlled and reversible modulation of conformational preferences of this photo-responsive ortho-azobenzene/2,6-pyridyldicarboxamide heterofoldamer has been established using UV/Vis, circular dichroism (CD) and 1H NMR spectroscopy. Additionally, the robust nature of the molecular, stimuli-induced, conformational switching events demonstrated by this photo-responsive scaffold, has been identified, with low levels of fatigue being observed within the system, even upon multiple cyclic treatments with irradiative and non-irradiative conditions.
To accommodate these key design considerations, a simple heterofoldamer design strategy, based on incorporating two well-established fold-promoting motifs of ortho-azobenzene and 2,6-pyridyldicarboxamide monomers, into the backbone of the foldamer was employed (Fig. 1). Crucially, the ortho-azobenzene units in 1 adopt the E-geometrical isomer under non-irradiative conditions which promotes the formation of a helical structure in the foldamers, whilst photo-induced isomerisation of the azobenzene units to the Z-isomer perturbs the helical the scaffold leading to a partially unfolded state upon the application of light.10,11 The helical conformation of 1 is further supported by the inclusion of the central 2,6-pyridyldicarboxamide unit, whose adoption of a syn–syn conformation is a fold-promoting motif commonly used in aromatic oligoamide foldamers and related photo-responsive heterofoldamers (Fig. 1).18,22 Moreover, the well-established reversible and robust nature of the stimuli-induced isomerization of azobenzene units provides the potential for the scaffold to demonstrate the desired repetitive photo-driven conformational switching behaviour with low levels of fatigue.10,11 In 1, (S)-(+)-naproxen groups are incorporated at the termini of the scaffold to bias the system towards the preferential adoption of one helical screw-sense. The positioning of the enantiopure groups at the termini of the scaffold ensures that the conformational preferences of the two fold-promoting motifs, ortho-azobenzene and the 2,6-pyridyldicarboxamide, are not perturbed and, hence, that a stable helical conformation is adopted by the scaffold in the absence of light.
Compound 1 was readily synthesized from 2-aminoacetanilide 2 in a five-step procedure (Scheme 1). Firstly, the treatment of 2 with oxone in a biphasic solvent mixture of dichloromethane/water, led to conversion of the amine group to the corresponding nitroso group, generating 3 as a bright green solid in 71% yield.23,243 underwent a Baeyer–Mills reaction with o-phenylenediamine upon refluxing in toluene, in the presence of acetic acid, to afford 2-acetamido-2′-amino-ortho-azobenzene 4 in 68% yield.23 Treatment of 4 with 2,6-pyridinedicarbonyl chloride, in the presence of pyridine, generated the acetyl terminated oligomer 5 as a bright orange solid in 52% yield. Removal of the acetyl protecting groups in 5 was achieved upon treatment with KOH in an acetone/water/methanol solvent mixture to give the corresponding diamine 6 in 45% yield. The diamine was reacted with an excess of (S)-(+)-naproxen chloride in the presence of pyridine to give 1 in 72% yield.
The importance of the two structural fold-promoting design features, of E-geometries of the azobenzene units and syn–syn conformation of 2,6-pyridyldicarboxamide unit in the backbone of the heterofoldamer scaffold of 1 is observed in the solid state. The adoption of the latter fold-promoting motif,20,25 results in the pyridyl amide protons being directed in towards the central cavity of the helix, leading to the formation of an intramolecular bifurcated hydrogen-bonding interaction26 involving the pyridyl N atom and the NH's of the adjacent amide bonds as anticipated (2.706(7)–2.742(7) Å, see Fig. S27 and S28†).27 In the crystal lattice of 1, the helices that aligned in columnar stacks orientated along the a axis (Fig. 2b). This crystal packing arrangement is supported by a diverse array of intermolecular non-covalent interactions formed between molecules within the same and adjacent columnar stacks including, C–H⋯O hydrogen bonding interactions28 involving aromatic and aliphatic protons and the O atoms of the carbonyl groups in neighbouring molecules, off-set π–π stacking interactions29 and C–H⋯π interactions30 (see ESI, Fig. S38–49†). Additionally, there are three intermolecular Cl3C–H⋯O hydrogen-bonding interactions31 involving chloroform solvent molecules and O atoms on the carbonyl group of amide bonds in 1 (see ESI, Fig. S50–52†).
Due to the presence of the azobenzene units in the backbone of the scaffold, 1 exhibits a UV/Vis absorption spectrum that displays a strong π → π* band at 412 nm which overlaps with the n → π* band at 464 nm (Fig. 3). The presence of the pyridyl carboxamide and the naproxen carboxamide groups at the ortho positions of the azobenzene units in 1 causes a larger red shift of the π → π* band compared to unsubstituted E-azobenzene, where it typically occurs at 320 nm. Accordingly, the photo- and thermally-driven configurational E/Z isomerization of the azobenzene units in 1 was studied using UV/Vis spectroscopy. Irradiation of a 4.8 × 10−5 M acetonitrile solution of 1 with 365 nm light induces photo-driven E → Z isomerization of the azo bonds in 1 as demonstrated by the observed decrease in the 412 nm and 464 absorption bands and an observed increase in the 530 nm absorption band corresponding to the Z isomer (Fig. 3).32 A photostationary state (PSS) is reached within 10 min of irradiation and thermal Z → E isomerization of the azo bonds in 1 proceeded over 220 min at ambient temperature, whereupon the reversibility of the photo-switching event was established through complete restoration of the initial UV/Vis signal obtained before irradiation (see Fig. 3).
To gain a better understanding of the photo-driven isomerization processes in 1, 1H NMR spectroscopy was used to follow the stimuli-driven molecular switching event. Irradiation of a 1.1 mM CD3CN sample of 1 with 365 nm light, for 45 min, afforded a PSS (Fig. 4b). Analysis of the 1H NMR spectrum of the PSS showed that, due to the presence of two azo bonds in the scaffold, three isomers (E/E, Z/Z and E/Z) of 1 were generated under irradiative conditions in 28%, 30% and 42% respectively.33 The symmetrical E/E and Z/Z-isomers of 1 display a single resonance for the NH amide proton of the carboxamide unit, Hc, at δ 11.20 ppm and δ 10.39 ppm respectively, wherein the Z-isomer displays significant upfield shifting of δ 0.81 ppm compared to the E-isomer (Fig. 4b).18a Whilst the asymmetrical E/Z isomer of 1 observed in the PSS, displays two resonances corresponding to the NH amide of the carboxamide unit, Hc, at δ 11.33 ppm (in the E-form) and at δ 10.52 ppm (in the Z-form) (Fig. 4b). Thermal Z → E isomerization of 1 occurred at ambient temperature over 285 min as determined by restoration of the original 1H NMR spectrum obtained before exposure to irradiative conditions (Fig. 4a–h).34 The Z isomer exhibited a half-life for the thermally-promoted Z → E isomerization of ∼ 100 min at 298 K (see ESI†).
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Fig. 4 Partial 1H NMR spectra (500 MHz, 298 K, CD3CN) of 1.1 mM solution of 1 showing the photo-driven E → Z isomerisation of the azobenzene units within the scaffold: (a) before irradiation, (b) PSS obtained after 45 min irradiation of the sample at 365 nm, (c) 45 min after initial irradiation of the sample, (d) 105 min after initial irradiation of the sample, (e) 135 min after initial irradiation of the sample, (f) 195 min after initial irradiation of the sample, (g) 225 min after initial irradiation, (h) 285 min after initial irradiation, (i) PSS obtained after fourth treatment of the sample with irradiative conditions at 365 min for 45 min (with 285 min thermal relaxation time allowed between each of treatments with irradiative conditions), (j) 280 min after fourth treatment with irradiative conditions. The NH amide proton of the carboxamide unit in 1, HC, is highlighted with the assignments corresponding to the lettering shown in Scheme 1. |
To obtain further information about the stimuli-induced changes on the global helical conformational switching behaviour of 1, CD spectroscopy was employed to monitor the system. The CD spectrum of a 6.7 × 10−5 M acetonitrile solution of 1 displays a large minima centred around 472 nm which is in the absorption region associated with the azobenzene units of the scaffold and a maxima centred at 394 nm which is in the absorption region associated with the azobenzene and oligoamide units of the scaffold.18c Accordingly, the observed CD signal indicates the presence of stable secondary helical conformation in solution in 1 in the absence of irradiative conditions (Fig. 5, blue line).18c The signs of the Cotton effects for the peaks at 472 and 394 nm (negative and positive respectively) are indicative of the preferential adoption of P-helicity by 1 in solution and aligns well with conformational preferences observed in the solid state.34 It is the presence of the terminal chiral (S)-(+)-naproxen groups in 1, that shift the equilibrium between left- and right-handed helical conformations, giving the rise to the preferential adoption of one helical screw-sense over the other and, thus leading to the observed CD signals associated with its secondary structure. Irradiation of a 6.7 × 10−5 M acetonitrile solution of 1 with 365 nm, for 10 min, afforded a PSS wherein a significant reduction in the magnitude of the Cotton effects in the negative peak at 472 nm (from −57.8 mdeg to −14.4 mdeg) and the positive peak at 394 nm (from 25.6 mdeg to 1.6 mdeg) (see Fig. 5, dashed red line) is observed. The observed photo-induced changes to these peaks in the CD spectrum of compound 1, indicates a conformational change is seen within the scaffold under irradiative conditions. This photo-induced change could be caused by depopulation of the helical conformation of the scaffold, due to the controlled local photo-induced E → Z isomerization of the azobenzene linkages in the backbone of the system (i.e., helix-coil transition), aggregation of the foldamer in this solvent and/or it could be caused by photo-induced re-orientation of the terminal naproxen group causing a change in the helical twist sense bias of the system (i.e., through chirality transfer from the naproxen-capping group to the foldamer chain).35 Whilst the latter case could be at least, in part, responsible for the observed photo-induced changes in the CD signal, controlled photo-induced conformational changes, in related azobenzene-based foldamers, are often attributed to structural helix-coil transitions.18c,36 Moreover, these literature reports combined with the pronounced conformational switching behaviour observed in 1 by 1H NMR spectroscopy (Fig. 4 and ESI), wherein significant shifting is observed for many of the signals of 1 upon irradiation which indicates that a large conformational change is induced across the whole of the foldamer, suggests that the significant changes observed by CD spectroscopy are likely to be at least, in part, caused by light-driven conformational switching from a globally stable well-folded helix to a partially unfolded scaffold. Thermal Z → E isomerization of the azo bonds in 1 occurs at ambient temperature to completely restore the initial CD signal, after 230 min, indicating regeneration of the original well-folded helical conformation of 1 under non-irradiative conditions (see Fig. 5).
Footnote |
† Electronic supplementary information (ESI) available: Full characterisation of new compounds as well as crystallographic data for compounds 1 and 4. CCDC 2121319 (1) and 2130347 (4). For ESI and crystallographic data in CIF or other electronic format see DOI: https://doi.org/10.1039/d3ob01137b |
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