Merve Basak Canalp and
Wolfgang H. Binder*
Faculty of Natural Science II (Chemistry, Physics and Mathematics), Martin Luther University Halle-Wittenberg, von-Danckelmann-Platz 4, Halle (Saale) D-06120, Germany. E-mail: wolfgang.binder@chemie.uni-halle.de
First published on 7th January 2020
Hybrid polymers of peptides resembling (partially) folded protein structures are promising materials in biomedicine, especially in view of folding-interactions between different segments. In this study polymers bearing repetitive peptidic folding elements, composed of N-terminus functionalized bis-ω-ene-functional oligo-L-lysine(carboxybenzyl(Z))s (Lysn) with repeating units (n) of 3, 6, 12, 24 and 30 were successfully synthesized to study their secondary structure introduced by conformational interactions between their chains. The pre-polymers of ADMET, narrowly dispersed Lysns, were obtained by ring opening polymerization (ROP) of N-carboxyanhydride (NCA) initiated with 11-amino-undecene, following N-terminus functionalization with 10-undecenoyl chloride. The resulting Lysns were subsequently polymerized via ADMET polymerization by using Grubbs’ first generation (G1) catalyst in 1,1,1,3,3,3-hexafluoroisopropanol (HFIP) generating the ADMET polymers (A-[Lysn]m) (m = 2–12) with molecular weights ranging from 3 to 28 kDa, displaying polydispersity (Đ) values in the range of 1.5–3.2. After chemical analyses of Lysns and A-[Lysn]ms by 1H-NMR, GPC and MALDI-ToF MS, secondary structural investigations were probed by CD spectroscopy and IR spectroscopy in 2,2,2-trifluoroethanol (TFE). In order to study A-[Lysn]ms with defined molecular weights and low polydispersity values (Đ = 1.03–1.48), the ADMET polymers A-[Lysn=3]m=3 and A-[Lysn=24]m=4 were fractionated by preparative GPC, and subsequently analysed by 1H-NMR, analytical GPC, MALDI-ToF MS and CD spectroscopy. We can demonstrate the influence of chain length of the generated polymers on the formation of secondary structures by comparing Lysns with varying n values to the ADMET-polymers with the help of spectroscopic techniques such as CD and FTIR-spectroscopy in a helicogenic solvent.
Various hybrid polymers containing poly-L-lysine/lysine(Z) with defined architectures, i.e., block copolymers, have been synthesized to integrate the biochemical features, e.g. pH responsivity, α-helicity within the synthetic polymer chain, and therewith assess and control functionality of the assembly formation. Diblock copolymers of polyisoprene-block-poly-L-lysine/lysine(Z) have been synthesized by combination of anionic polymerization and ROP methods to obtain ‘‘hybrid’’ rod–coil block copolymers based on a synthetic coil segment and a polypeptide chain, displaying an α-helical conformation for use in nanotechnology.27 Poly(styrene)388-block-poly(L-lysine)138 diblock copolymer changes its assembly to form pH responsive aggregate when mixed with a non-ionic surfactant, such as C12E6.28 The secondary structure of poly(butadiene)107-block-poly(L-lysine)27 has been probed by CD spectroscopy as a function of pH and temperature, suggesting that an α-helix of the poly(L-lysine) block transforms into β-sheets at higher temperature (T = 60 °C) at a pH = 11.2.29 Another study has yet adjoined the secondary structural features of poly(L-lysine), combined with the thermo-responsive behaviour of poly(N-isopropylacrylamide) to achieve amphiphilic hybrid rod-coil block copolymers by combination of atom transfer radical polymerization (ATRP) and ROP.30
In this work it was aimed to combine the variable secondary structure of the oligo-L-lysine(Z) in combination with ethylene chains in a repetitive manner to investigate secondary structural changes such as α-helicity induced assemblies of the so obtained hybrid polymers as represented in Fig. 1. Based on a combination of NCA ROP of N-carboxyanhydrides and ADMET polymerization techniques it is aimed to obtain hybrid polymers with the desired peptide/ethylene units, based on ADMET polymers of oligo-L-lysine(Z)s (green in Fig. 1). As the intermediate oligo-ethylene-segments (shown in grey, Fig. 1) can be considered as noninteracting in the sense of a supramolecular interaction, the so chosen molecular design allows to primarily study the intersegmental interactions of the (partially) folded oligo-L-lysine(Z)s, probed by CD- and IR-methods in TFE. In order to obtain reliable information as to the conformational status of the oligo-L-lysine(Z)s-segment, careful fractionation by preparative GPC was accomplished to enable a detailed study of the intersegmental conformational changes.
Entry | Pre-polymers (Lysn) | ADMET polymers (A-[Lysn]m) | Solvent | Catalyst | DPNMR (n, m) | Mn, GPC [kDA] | Đ |
---|---|---|---|---|---|---|---|
I | Lysn=3 | A-[Lysn=3]m=3 | HFIP | G1 | 4, 3 | 3.7 | 2.2 |
II | Lysn=3 | A2-[Lysn=3]m=2 | HFIP | G1 | 4, 2 | 2.9 | 1.5 |
III | Lysn=6 | A-[Lysn=6]m=12 | HFIP | G1 | 6, 12 | 11.2 | 3.2 |
IV | Lysn=6 | A2-[Lysn=6]m=2 | HFIP | G1 | 6, 2 | 3.7 | 1.4 |
V | Lysn=6 | A3-[Lysn=6]m=18 | TFE | G1 | 6, 18 | 20.9 | 4.8 |
VI | Lysn=12 | A-[Lysn=12]m=8 | HFIP | G1 | 12, 8 | 15.7 | 2.4 |
VII | Lysn=24 | A-[Lysn=24]m=4 | HFIP | G1 | 24, 4 | 10.6 | 1.7 |
VIII | Lysn=24 | A2-[Lysn=24]m=3 | HFIP | G1 | 24, 3 | 7.5 | 1.5 |
IX | Lysn=30 | A-[Lysn=30]m=7 | HFIP | G1 | 30, 7 | 27.8 | 2.4 |
The ROP of NCA monomers is a viable and proven strategy to obtain artificial homo- and block co-peptides, where end group functionalized polymers can be obtained, given that the ROP mechanism follows the aspects of “livingness”.40,41 Firstly, mono-functional oligo-L-lysine(Z)s with varying repeating units (n = 3, 6, 12, 24, 30) were synthesized via ROP of the lysine-NCA monomer using 11-aminoundece as the primary initiator in DMF. It has been known that livingness and end group fidelity during ROP of NCAs can be achieved via the “Normal Amine Mechanism (NAM)” using primary or secondary amines as initiators.20,42–44 Therefore the NCA monomer of N-carboxybenzyl(Z)-L-lysine amino acid, NCA(Z), was initiated via the primary amine, 11-aminoundecene, to obtain the mono-functional oligo-L-lysine(carboxybenzyl(Z))s in the first step. After proving the chain length and end groups via NMR- and MS-analyses (see ESI†), the N-terminal end groups were functionalized by direct amidation with 10-undecenoyl chloride in situ to achieve the respective bis-ω-ene-functional pre-polymers, Lysns.22
Relying on the excellent possibilities of ADMET polymerization to include amino acids onto a polyolefin chain,45–47 the Lysns (n = 3, 6, 12, 24, 30) were further polymerized by ADMET polymerization in HFIP by addition of Grubb's first generation catalyst (G1) (see Scheme 1 and Table 1). All obtained Lysns and A-[Lysn]ms were characterized by 1H-NMR, MALDI-ToF MS and analytical GPC (see Table 2 and ESI†). Additionally, the ADMET polymers A-[Lysn=3]m=3 and A-[Lysn=24]m=4 were fractionated by preparative GPC and then selectively investigated by MALDI-ToF MS, analytical GPC, 1H-NMR (see Table 2, Fig. 2, 3 and ESI†). Structural investigations of Lysns, A-[Lysn]ms and the selected fractions of A-[Lysn]ms were mainly done by CD spectroscopy in TFE (see Table 2, Fig. 4, 5 and also ESI†). IR spectroscopy in TFE was also probed to analyse secondary structure features of Lysns and A-[Lysn]ms (see Fig. 6 and ESI†).
Scheme 1 Schematic representation of the synthetic pathway of ADMET polymerization of Lysn22 by using Grubb's first catalyst (G1). |
Entry | Samples | DPtheo. (n) | DPNMR (n, m) | Mn, MALDI [kDA] | Mn, GPC in DMF [kDA] | Đ | CD-Spec. (in TFE) |
---|---|---|---|---|---|---|---|
Oligo-L-lysine(Z)s | |||||||
I | Lysn=3 | 3 | 4 | 2.2 ± 1.8 | 1.9 | 1.06 | β II turn |
II | Lysn=6 | 6 | 6 | 3.2 ± 1.6 | 2.8 | 1.17 | 25% α-helicity |
III | Lysn=12 | 12 | 11 | 3.3 ± 1.7 | 3.3 | 1.36 | 27% α-helicity |
IV | Lysn=24 | 24 | 23 | 3.6 ± 1.2 | 6.3 | 1.40 | 53% α-helicity |
V | Lysn=30 | 30 | 30 | 5.6 ± 4 | 8.0 | 1.33 | 65% α-helicity |
ADMET polymers of oligo-L-lysine(Z)s & the selected fractions | |||||||
VI | A-[Lysn=3]m=3 | 3 | 3 | 2.5 ± 1.2 | 3.7 | 2.20 | β II turn |
VII | F10 + 11 + 12 | 3 | NA | NA | 23.2 | 1.21 | 18% α-helicity |
VIII | F13 + 14 | 3 | NA | 8.1 ± 3 | 12.8 | 1.12 | 15% α-helicity |
IX | F15 | 3 | NA | 6.5 ± 2 | 9.2 | 1.08 | β II turn |
X | F17 | 3 | NA | 2.8 ± 1.7 | 5.8 | 1.05 | β II turn |
XI | F18 | 3 | NA | 2.6 ± 1.6 | 4.7 | 1.05 | β II turn |
XII | F21 + 22 + 23 | 3 | NA | 2.6 ± 0.5 | 2.6 | 1.04 | β II turn |
XIII | F24 + 25 | 3 | NA | 2.1 ± 0.5 | 2.1 | 1.03 | β II turn |
XIV | A-[Lysn=6]m=12 | 6 | 12 | 4.3 ± 2.5 | 11.2 | 3.21 | 32% α-helicity |
XV | A-[Lysn=12]m=8 | 12 | 8 | 4.7 ± 3.2 | 15.7 | 2.43 | 44% α-helicity |
XVI | A-[Lysn=24]m=4 | 24 | 4 | 4.1 ± 2.4 | 10.6 | 1.74 | 69% α-helicity |
XVII | F12 | 24 | NA | NA | 23.2 | 1.16 | 77% α-helicity |
XVIII | F13 | 24 | 4 | NA | 19.1 | 1.15 | 62% α-helicity |
XIX | F15 | 24 | NA | 14.2 ± 2 | 12.1 | 1.07 | 53% α-helicity |
XX | F16 | 24 | NA | 13.7 ± 2 | 10.9 | 1.07 | 52% α-helicity |
XXI | F18 | 24 | NA | 7.7 ± 2 | 7.1 | 1.08 | 40% α-helicity |
XXII | A-[Lysn=30]m=7 | 30 | 7 | 4.3 ± 2 | 27.8 | 2.41 | 79% α-helicity |
Fig. 2 Preparative GPC graphs of (a) A-[Lysn=3]m=3 (b) A-[Lysn=24]m=4 along with their analytical GPC results of respective (c) fractions of A-[Lysn=3]m=3 and (d) fractions of A-[Lysn=24]m=4. |
Fig. 3 MALDI-ToF MS spectra of (i) A-[Lysn=24]m=4 before fractionation along with the simulated isotopic patterns (reflector mode) and (ii) the selected fractions of A-[Lysn=24]m=4 (linear mode) (also see ESI†). |
Fig. 4 CD spectra of (a) Lysn=6, A-[Lysn=6]m=2, A-[Lysn=6]m=12 (b) Lysn=12, A-[Lysn=12]m=8 (c) Lysn=24, A-[Lysn=24]m=3, A-[Lysn=24]m=4, (d) Lysn=30 and A-[Lysn=30]m=7. (c = 2 mg mL−1 in TFE). |
Fig. 5 CD spectra of fractions of (a) A-[Lysn=3]m=3 (F10 + 11 + 12, F13 + 14, F15, F17, F18, F21 + 22 + 23, F24 + 25) and (b) A-[Lysn=24]m=4 (F12, F13, F15, F16, F18). (c = 2 mg mL−1 in TFE). |
Fig. 6 IR spectra of ADMET polymers A-[Lysn=3]m=3, A-[Lysn=12]m=8 and A-[Lysn=30]m=7 (c = 5 mg mL−1 in TFE). |
Thus, ADMET polymers A-[Lysn=3]m=3 (Table 2, entry VI) and A-[Lysn=24]m=4 (Table 2, entry XVI) were separated into fractions (Table 2, entries VII–XIII for the former and Table 2, entries XVII–XXI for the letter) according to their molecular weights, thus displaying significantly lower Đ values than their native unfractionated samples via preparative GPC technique in DMF at a column temperature of 55 °C.
Preparative GPC traces of A-[Lysn=3]m=3 (Fig. 2a) and A-[Lysn=24]m=4 (Fig. 2b) along with the analytical GPC results of their fractions (Fig. 2c and d respectively) are demonstrated. As depicted in Fig. 2a and b, all fractions are named as Fx, i.e., x is the alignment number of the fraction trace in the preparative GPC graph. The complete analytical GPC results of all the fractions of A-[Lysn=3]m=3 (Table 1S†) and A-[Lysn=24]m=4 (Table 2S†) are present within the ESI.†
As can be seen from the obtained analysis results, molecular weights of fractions of ADMET polymer A-[Lysn=3]m=3 (Table 2, entry VI) increases with the decreasing number of the fraction trace number, e.g. F25 (Mn ≈ 2 kDa) and F15 (Mn ≈ 10 kDa) (see ESI, Table 1S†). All obtained fractions of A-[Lysn=3]m=3 measured by analytical GPC in DMF display low Đ values (1.20 > Đ > 1.03) which proves the successful separation of the fractions.
In the case of the high molecular weight ADMET polymer, A-[Lysn=24]m=4 (Table 2, entry XVI), molecular weight of the fractions also increases with the decreasing number of the fraction trace number, e.g. F18 (Table 2, entry XXI) (Mn ≈ 7.2 kDa) and F10 (Mn ≈ 23 kDa) (see ESI, Table 2S†). All obtained fractions of A-[Lysn=24]m=4 measured by analytical GPC in DMF have low Đ values (1.48 > Đ > 1.07) when they are compared with ADMET polymers which have Đ values over 2.0 in general.
In Fig. 3, the measured MALDI-ToF MS spectra of A-[Lysn=24]m=4 before fractionation with the simulated isotopic patterns (Fig. 3i) and after fractionation of selected fractions of A-[Lysn=24]m=4, i.e., F14–F18 (Fig. 3ii) are shown. The measured MALDI spectra and the respective simulated isotopic patterns of A-[Lysn=24]m=4 (Fig. 3i) prove the ADMET polymer structure, having –CH2 characteristic difference due to the fragmentated isomers of ADMET polymers, where the simulated and the measured spectra match. Similar to the analytical GPC investigations, the measured MALDI spectra of selected fractions of A-[Lysn=24]m=4 in Fig. 3ii verify the increasing molecular weight of the fractions with decreasing fraction trace number obtained by preparative GPC (see Fig. 2 and also ESI, Table 2S†). According to the measured MALDI spectra in Fig. 3ii, F14 has a molecular weight of ≅16 ± 3 kDa whereas the low molecular weight fraction F18 has a molecular weight of ≅7 ± 3 kDa, which evidences an average molecular weight difference of 9 kDa. Therefore, all these fractional analyses of ADMET polymers are suited for the subsequent secondary structural investigations.
Enhanced α-helicity with increasing n number was observed for oligo-L-lysine(Z)s Lysns (see Table 2, and ESI Fig. 20S†) as also supported by our previous investigations.22 As an example, Lysn=6 (Table 2, entry II) displays 25% α-helicity, while Lysn=30 (Table 2, entry V) with its higher degree of polymerization displays 65% α-helicity. Similarly, structural investigations utilizing CD spectroscopy have also been probed by Huesmann et al.20 where mono-functional poly-L-lysine(Z)s prepared by hexylamine with n = 24, 57, 87, 196 (Đs ∼ 1.70) have been investigated in HFIP. According to their investigations, poly-L-lysine(Z) with n = 5–15 did not display an ordered secondary conformation, however only at a chain length of n ≈ 60 α-helicity was observed, thus showing an increase in helicity with increasing n.
Secondly, the effects resulting from repetition of the helical segments on the secondary structure formation was investigated by the comparison of the oligomers and their respective ADMET polymer derivatives. Thus, the measured CD spectra of the oligomers along with their respective ADMET polymers are given in Fig. 4. In this regard, since the helical segments are repetitively present within the hybrid polymers of A-[Lysn]ms (n > 4), it is observed from the increasing intensities of [θ]222 from Fig. 4 that their α-helicity values increase from around 30 to 80 percentage (see Table 2, entries XIV, XV, XVI and XXII). To exemplify, Lysn=24 (Table 2, entry IV) displays ∼ 53% α-helicity, and on the other hand the respective ADMET polymer of Lysn=24, A-[Lysn=24]m=4 (Table 2, entry XVI), displays around 69% α-helicity. ADMET polymer of Lysn=30, A-[Lysn=30]m=7 (Table 2, entry XXII), in a similar way, shows a higher tendency to form helical structure which increases from 65 to 79% α-helicity. Both results point at an interference of the individual Lysn – blocks along the ADMET-polymers, leading to a distinct increase of their helicity.
It also was of interest to investigate the effects of the chain lengths of the ADMET polymers on the formation of α-helices. Therefore, selected fractions of ADMET polymers, namely A-[Lysn=3]m=3 (Table 2, entry VI) and A-[Lysn=24]m=4, were examined by CD spectroscopy in TFE. From the CD measurements represented in Fig. 5 and the calculations of α-helicity percentage values given in Table 2, one can deduce that the overall molecular weight of the hybrid polymers, and thus, the repeating unit of L-lysine(Z) moieties plays a decisive role in forming α-helices. Before fractional analyses, as it was expected, ADMET polymer A-[Lysn=3]m=3, did not show any α-helicity due to its low number of L-lysine(Z) units, devoid of a stabilization of a proper helical turn.51,52 However, after fractionation of A-[Lysn=3]m=3, α-helicity could be observed from CD spectroscopy measurements done in TFE, where the obtained fractions F10–12 (Table 2, entry VII) and F13–14 (Table 2, entry VIII) show around 15–18% α-helicity as it is also shown in Fig. 5a. Furthermore, some selected fractions of A-[Lysn=24]m=4 were also investigated by CD as shown in Fig. 5b. The signal intensities at 222 nm, [θ]222, get even more significant for the fractions of A-[Lysn=24]m=4 as the molecular weight of the fraction increases from F18 (Table 2, entry XXI) to F12 (Table 2, entry XVII), again proving that α-helicity propensities increase with the increasing molecular weight of the hybrid polymer.
Last but not least, the molecular weight dependence on the secondary structural features of the selected fractions of both A-[Lysn=3]m=3 and A-[Lysn=24]m=4 could also be compared. For instance, F10 + 11 + 12 (Table 2, entry VII) and F12 (Table 2, entry XVII) display the same Mn values (23.2 kDa), however the former one shows only around 18% α-helicity whereas the letter has around 77% α-helicity. Similarly, comparing the α-helicity percentage values of F13 + 14 (Table 2, entry VIII) with F15 (Table 2, entry XIX) and F15 (Table 2, entry IX) with F16 (Table 2, entry XX) indicates that not only the molecular weights of the hybrid polymers but also the number of repeating units of L-lysine(Z) along the whole chain plays a significant role in their secondary structural properties, i.e., their α-helicity propensities.
Furthermore, infrared (IR) spectroscopy, which is a well-known and versatile experimental technique to analyse chemical as well as biological samples either in solution or in the solid state, was additionally employed.19,53,54 With the help of IR spectroscopy measurements, it was intended to gain insight into the presence of the other common secondary structures, e.g., β-sheets and β-turns. However, owing to the sufficient solubility of only some of the samples, we could obtain structural investigations by IR spectroscopy in only partial depth (see ESI†).
With the help of IR, one can observe secondary structures which produce characteristic electron densities in the amide CO groups, giving rise to distinctive amide I frequencies (1620–1700 cm−1) in the IR spectra. Since the length of the hydrogen bond resulting from α-helix conformation formed by the CO group of the residue n positioned to interact intramolecularly with the N–H group of the residue n + 4 will be slightly longer (and thus weaker) than that of in a β-sheet structure, it gives further increase in amide I frequency.53,55 Concordantly, α-helix structures contribute to amide I frequency signals at around 1648–1660 cm−1, while β-sheet structures are observed at around 1625–1640 cm−1.56
IR spectra of ADMET polymers, A-[Lysn=3]m=3 are shown with a yellow line, A-[Lysn=12]m=8 with a black line and A-[Lysn=30]m=7 with a blue line are shown in Fig. 6. As previously observed from CD investigations in TFE, α-helicity structure formation tendency increases with the increasing number of repeating units (n) which could be also observed from the intense sharp peak of the blue line at ≈1650 cm−1 proving α-helicity of the ADMET polymer (A-[Lysn=30]m=7) in IR spectra. Since the number of repeating units of peptide decreases, as seen in the cases of ADMET polymers, A-[Lysn=12]m=8 and A-[Lysn=3]m=3, the IR signal at ≈1650 cm−1 get weaker and broader most probably because of the presence of other unordered structure. The signals at around 1700 cm−1 stem from the dynamic nature of secondary structure formation resulting in different secondary structural features such as β-sheets and β-turns.
In order to work up a connection in between secondary structures of different types of hybrid polymers such as linear peptides with β-turn motifs in TFE57 and amyloid-type fibrils with β-sheet structures in solution, CD and IR methods have been used jointly.58 Consequently, IR measurements assist the secondary structural analyses performed by CD spectroscopy, while the latter provides more accurate estimations of α-helix content and the former one is more sensitive to β-sheets.59 In comparison to IR measurements, our CD investigations performed in TFE help us quantify α-helicity of the oligomers and the ADMET polymers straightforwardly as shown in Fig. 4 and 5b and Table 2. Hence, in an attempt to indicate the presence of β-sheets and β-turns, especially in the case of highly α-helical polymers, e.g., A-[Lysn=30]m=7, we employed IR as shown in Fig. 6. Similarly, another study has utilized both IR and CD methods and reported that at native pH, lipopeptides form β-sheet nanofibers in aqueous solution with a strong IR peak at 1616–1620 cm−1 and CD spectra displaying similar characteristic signals of a β-sheet secondary structure, i.e., minima at ∼216 nm and a maximum at ∼197 nm.60
To this date, the features determining the folding behaviours of helix bundles, e.g., four-helix bundle motifs, have been drawn upon as a model for understanding the forces governing functional protein folding such as in the case of transmembrane protein GLUT1.61–63 According to the findings the burial of hydrophobic residues, conformational entropy, packing constraints, helix dipole and interhelical turns have an impact on forming such helix–helix bundles. Additionally, it has been known that the perfectly ordered biologically active three-dimensional structures of proteins form such functional assemblies by the interplay of varying interactions, e.g., noncovalent interactions.64,65 These noncovalent cooperative interactions are mainly interpreted from their hydrogen bonding affinities.66,67 Similar to our current study model helical polymers, studied under different conditions to examine their helix–coil transitions, also showed changes in secondary structure induced by the repeating number of helical chains, i.e., length and strength of helices.68–70 Based on CD and IR-measurements in our study we can also prove a change of helical structures induced by chain length (n), end chain moieties and helicogenic solvent effects. In summary, our secondary structural investigations in TFE revealed that ADMET polymers have higher propensities than the oligomers to exhibit and stabilize α-helical structure, proposed as a result of the packing of their repetitive helical segments present within the hybrid polymer chain that form intramolecular interactions of the hydrogen bonding moieties, namely L-lysine(Z)s, once the α-helix structure has been provided (n > 4).
The secondary structural investigations were conducted with the help of CD spectroscopy and IR spectroscopy in TFE. Throughout our secondary structural investigations, we intended to draw attention to the effects of number of chains (n) of Lysns, as reported in our preceding work, and of their ADMET derivatives, i.e., A-[Lysn]ms, in an α-helix promoting solvent. Our secondary structural investigations have shown that an increasing number of peptide unit increases the propensity to form α-helices. This phenomenon can be better understood by comparing the CD spectra of the fractions of A-[Lysn=3]m=3 and A-[Lysn=24]m=4 selectively investigated by CD spectroscopy in TFE, proving the effects of the controlled molecular weights with low Đ values of the hybrid polymers on the formation of α-helices. Thus, the individual oligomers, the Lysn segments, do interact along the main chain, inducing increased helicity with increasing chain length of the overall ADMET polymer. It can be proposed that this type of cooperative phenomenon is similar to other multi-folded proteins, where close proximity between individual segments can change the overall conformation of individual part – e.g. in globular proteins with helix–helix interaction motifs, as common for many transmembrane proteins. We think that these polymers can serve as a model-system to study influences from distance-related folding and refolding phenomena.
Footnote |
† Electronic supplementary information (ESI) available: 1H-NMR, MALDI-ToF, CD, IR, etc. See DOI: 10.1039/c9ra09189k |
This journal is © The Royal Society of Chemistry 2020 |