Open Access Article
Merve Basak Canalpa,
Annette Meisterb and
Wolfgang H. Binder
*a
aFaculty 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
bInstitute of Biochemistry and Biotechnology, Martin Luther University Halle-Wittenberg, Kurt-Mothes-Straße 3a, Halle (Saale) D-06120, Germany
First published on 12th July 2019
Fibrillation of supramolecular building blocks represents an important model system for complex proteins and peptides, such as amyloidogenic proteins, displaying aggregation and subsequent collapse of their biological functions. In this work, we synthesized narrow-dispersed, end group-telechelic, oligomeric-(L-lysine(carboxybenzyl (Z)/trifluoroacetyl (TFA)))ns (n = 3–33) as a model system for studying assembly and secondary structure formation, prepared via ring opening polymerization (ROP) of N-carboxyanhydrides (NCA). Our primary goal was to understand the influence of amino acid chain length and end group-modification on the secondary structure and fibrillation of the oligo-Z/TFA-protected lysines. Synthesis was accomplished by initiation of ROP with 11-amino-undecene, followed by complete chain end functionalization reactions of the N-terminus by 10-undecenoyl-chloride. The so obtained oligomeric-(L-lysine(Z/TFA))ns were fractionated according to their number of repeating units (n) with preparative GPC using DMF as the eluent. As proven by MALDI-ToF MS, 1H-NMR-spectroscopy and analytical GPC, they were separated into fractions with low polydispersity (Đ) values, ranging from 1.02–1.08. Secondary structural investigations of these narrowly-dispersed oligomeric-(L-lysine(Z/TFA))ns (n = 33 ± 6, n = 18 ± 6, n = 12 ± 4, n = 5 ± 2) were accomplished by CD spectroscopy in TFE and HFIP, indicating that TFE was able to induce/stabilize the formation of α-helicity. Fibril formation of oligomeric-(L-lysine(Z/TFA))ns with shorter chain lengths (n = 7 and n = 3) were chosen to investigate the effect of the number of repeating units' role on the self-assembly of the oligomers in TFE. TEM images of these selected fractions, f19 with n = 7 and f28 with n = 3, showed that fibrillization occured and the formation of a dense fibrillar mesh was observed when the amino acid chain length is equal to 7. Therefore, the influences of the number of repeating units (n), end-group functionalities (mono- or bis-functional) and the choice of solvents (TFE or HFIP) on the propensity to form helical structure allowed us to calibrate their secondary structure.
Our study aims to investigate the secondary structural behaviour of: (i) the chain end effects introduced by C11 alkyl groups on each end of the peptide, similar to lipid/peptide hybrids in e.g. lipopeptides23 or peptide amphiphiles24,25 and (ii) investigate the influence of the side chain effects of the protecting groups, Z(Cbz) and TFA, exerted on the oligomeric lysines in solution. In order to get a deeper understanding of the effects of the number of repeating units (n) on the formation of helices and their fibrillation behaviour, we have fractionated the N-terminus functionalized oligomers, enabling us to perform investigations by CD in two different solvents (HFIP and TFE) with the aim to understand to what extent TFE can stabilize α-helix formation. We therefore have prepared oligomeric L-lysines with low molecular weights (Mn = 2–3 kDa) via ROP of NCA monomers using 11-aminoundecene as the primary amine initiator, followed by an additional chain end functionalization via amidation reaction of the amino group of the N-terminus with 10-undecenoyl chloride. Subsequently, fractionated samples of N-terminus functionalized oligomers obtained by preparative GPC were investigated by MALDI-ToF MS, analytical GPC and CD spectroscopy to study their conformational behaviour at precise chain lengths (n).
000 g mol−1 were used for external calibration. Preparative GPC was performed by a KD-2002.5 column from Shodex company attached on a VWR HITACHI Chromaster instrument using DMF (HPLC graded) as the eluent at 55 °C with a flow rate of 0.70 mL min−1 injecting sample with the concentration of 15 mg mL−1 where refractive index detector from VWR at 50 °C was employed as the detector. The obtained data were analysed by using EZChrom Elite (version 3.3.2 SP2) software. ESI-ToF measurements were performed on a Focus micro ToF by Bruker Daltonics. The sample (1.00 mg) was dissolved in methanol (1.00 mL, HPLC grade) and directly infused (180.00 μL h−1, positive or negative mode). MALDI-TOF MS measurements were carried out in reflector mode on a Bruker Autoflex III Smart beam equipped with a nitrogen laser source (λ = 337 nm). The samples were dissolved in DMF (HPLC grade) (c = 10 mg mL−1) with a ratio of 100
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10
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1 (matrix
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analyte
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salt). The matrix dithranol with c = 10 mg mL−1 in THF, the salt potassium trifluoroacetate (KTFA) with c = 5 mg mL−1 in THF were used. For the data evaluations and simulation of the mass spectra of the polymer samples the computer programme Flex analysis (version 3.0) was used. CD spectroscopy measurements were performed with the instrument, JASCO Corp., J-810, Rev. 1.00, at a constant temperature (20 °C). The UV absorption was measured in CD units of millidegrees in the wavelength range of 260–190 nm. The cuvette cell used had a diameter of 0.1 cm. The correction of the measurements was done by subtraction of the absorption of the pure solvents e.g. 1,1,1,3,3,3-hexafluoroisopropanol (HFIP) and 2,2,2-trifluoroethanol (TFE) from the absorbance of the sample. The negatively stained samples for Transmission Electron Microscopy (TEM) were prepared by spreading 5 μL of the dispersion (0.2 mg mL−1 in TFE) onto a Cu grid coated with a Carbon-film (PLANO, Wetzlar, D). After 1 min excess liquid was blotted off with filter paper and 5 μL of 1% aqueous uranyl acetate solution were placed onto the grid and drained off after 1 min. The dried specimens were examined with an EM 900 transmission electron microscope (Carl Zeiss Microscopy GmbH, Oberkochen, Germany). Micrographs were taken with a SSCCD SM-1k-120 camera (TRS, Moorenweis, Germany).
CH–CH2, 3,3,3JH,H = 13.5, 10.3, 6.7 Hz), 5.26–4.78 (m, 25H, CH2C
C, CH2), 4.42 (d, 9H, CH, 3JH,H = 6.7 Hz), 3.39–2.99 (m, 25H, CH2), 2.30–1.15 (m, 94H, CH2). MS (MALDI-ToF, Dithranol/KTFA): m/z calc. = 1518.8 [M + K]+, m/z exp. = 1519.0 [M + K]+.
CH–, 3,3JH,H = 16.6, 6.6 Hz), 4.95 (dd, 2H, CH2
CH–, 2,3JH,H = 30.2, 13.6 Hz), 4.79 (dd, 1H, CH, 3,3JH,H = 9.9, 5.4 Hz), 4.40 (m, 4H, CH), 3.43 (d, 18H, CH2, 3JH,H = 6.6 Hz), 2.14–1.15 (m, 51H, CH2). MS (MALDI-ToF, Dithranol/KTFA): m/z calc. = 1328.5 [M + K]+, m/z exp. = 1328.6 [M + K]+.
CH–, 3,3JH,H = 10.2, 6.8 Hz), 5.32–4.84 (m, 74H, H2C
C, CH2), 4.43 (s, 7H, CH), 3.24 (d, 2H, CH2, 3JH,H = 5.9 Hz), 2.48–1.05 (m, 340H, CH2). MS (MALDI-ToF, Dithranol/KTFA): m/z calc. = 1669.0 [M + K]+, m/z exp. = 1668.5 [M + K]+.
CH–, 3,3JH,H = 10.2, 6.8 Hz), 4.95 (dd, H2C
C, CH2), 4.43 (s, 7H, CH), 3.24 (d, 2H, Hd, i, CH2, 3JH,H = 5.9 Hz), 2.48–1.05 (m, 340H, CH2). MS (MALDI-ToF, Dithranol/KTFA): m/z calc. = 1494.7 [M + K]+, m/z exp. = 1494.7 [M + K]+.As presented in Fig. 1 and 2, both N-OK(Z) and N-OK(TFA) were fractionated successfully, see Fig. 1A and B, collecting the different fractions, labelled as fx. As can be seen from Fig. 1A, for N-OK(Z) 11 fractions (f) f12–f28 were collected, whereas the fractionation of N-OK(TFA) resulted only in 4 fractions which were referred to as f2 (n = 6), f3 (n = 5), f4 (n = 4) and f5 (n = 3) (Fig. 1B). After fractionation, all fractions were analysed by analytical GPC as shown in Fig. 1C (for N-OK(Z)) and Fig. 1D (for N-OK(TFA)), displaying significantly narrow polydispersity values as compared to the unfractionated samples, N-OK(Z) and N-OK(TFA). Subsequently, all selected fractions were also analysed by MALDI-ToF MS (see Fig. 2 and Table 1) as well as 1H-NMR spectroscopy (see Fig. 3).
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| Fig. 1 Preparative GPC graphs of (A) N-OK(Z), (B) N-OK(TFA) and analytical GPC graphs of (C) N-OK(Z), (D) N-OK(TFA) along with the selected fractions. | ||
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| Fig. 2 MALDI-ToF MS of (a) N-OK(Z), (b–f) fractions of N-OK(Z), (g) N-OK(TFA) and (h–k) fractions of N-OK(TFA). | ||
| Entry | Sample | n(MALDI) | Mn(MALDI) | Mn(GPC) | Đ | CD-spec. (HFIP) | CD-spec. (TFE) |
|---|---|---|---|---|---|---|---|
| I | OK(Z) | 15 ± 10 | 4.1 | 2.5 | 1.36 | 22% α-helicity | 32% α-helicity |
| II | N-OK(Z) | 15 ± 10 | 4.2 | 1.4 | 1.36 | 16% α-helicity | 19% α-helicity |
| III | N-OK(Z)-2 | 8 ± 2 | 2.1 | 1.9 | 1.02 | β II turn | 18% α-helicity |
| IV | N-OK(Z)-3 | 24 ± 8 | 5.6 | 8.0 | 1.33 | 40% α-helicity | 53% α-helicity |
| V | f12 | 33 ± 6 | 8.9 | 9.1 | 1.08 | 19% α-helicity | 32% α-helicity |
| VI | f14 | 18 ± 6 | 4.9 | 4.9 | 1.07 | 15% α-helicity | 25% α-helicity |
| VII | f15 | 12 ± 4 | 3.4 | 3.7 | 1.07 | β II turn | 18% α-helicity |
| VIII | f16 | 8 ± 2 | 2.3 | 2.6 | 1.02 | β II turn | 16% α-helicity |
| IX | f19 | 6 & 7 | 2.1 | 2.6 | 1.03 | β II turn | 16% α-helicity |
| X | f20 | 6 ± 2 | 2.1 | 2.6 | 1.03 | β II turn | 16% α-helicity |
| XI | f23 | 5 ± 1 | 1.8 | 2.3 | 1.03 | β II turn | 15% α-helicity |
| XII | f25 | 4 ± 1 | 1.5 | 2.0 | 1.03 | β II turn | 12% α-helicity |
| XIII | f28 | 3 | 1.1 | 1.8 | 1.02 | β II turn | 12% α-helicity |
| XIV | OK(TFA) | 6 ± 3 | 1.5 | 1.0 | 1.09 | 16% α-helicity | 31% α-helicity |
| XV | N-OK(TFA) | 6 ± 3 | 1.6 | 1.2 | 1.05 | β II turn | 15% α-helicity |
| XVI | f2 | 6 ± 1 | 1.4 | 1.3 | 1.02 | β II turn | 19% α-helicity |
| XVII | f3 | 5 ± 1 | 1.2 | 1.2 | 1.02 | β II turn | 15% α-helicity |
| XVIII | f4 | 4 ± 1 | 1.0 | 1.0 | 1.02 | β II turn | β II turn |
| XIX | f5 | 3 & 4 | 0.90 | 0.96 | 1.02 | β II turn | β II turn |
In Fig. 2, the MALDI spectra of both fractionated oligomers f28, f19, f15, f14, f12 of N-OK(Z) (b–f) and f5, f4, f3, f2 of N-OK(TFA) (h–k) along with the oligomers (a and g) before fractionation are shown. MALDI spectra prove that the fractions were well separated, with defined end group functionalities on both sides of the respective oligomers, as shown by the excellent match between the simulated and the measured isotopic patterns of the samples (see details in the ESI, Fig. 19S–29S and 31S–33S†). The analytical GPC results also support (see Fig. 2 and Table 1) the very narrow Đ values for each fraction with small variations in the numbers of repeating units (n). Thus, at n = 3 to 8 only a chain variation of ±2 was obtained, and at n = 12–33 the variation was ±6.
As shown in Fig. 3, we have investigated the fractions f12 and f28 of N-OK(Z) by 1H-NMR spectroscopy in CDCl3 (15% volume TFA added), proving their chemical identity and a good match to the data obtained by GPC and MALDI.
All analytical data of the samples are summarized in Table 1, along with the respective n, Mn and Đ values.
α-helix (%) = (−[θ]222 + 3000)/39 000 × 100%
| (1) |
The summary of all CD spectroscopy measurements along with analytical GPC results of oligomers and their fractions are presented in Table 1. The secondary structural investigations of the fractions of N-OK(Z); f28, f19, f15, f14, f12 and of N-OK(TFA); f4, f3, f2 in TFE are depicted in Fig. 4A and B respectively (also see Table 1).
Firstly, we investigated the effect of the number of repeating units (n) on formation of secondary structures by CD spectroscopy, aiming to understand changes in α-helicity with increasing chain length n of the bis-substituted N-OK(Z) oligomers (Fig. 4A and Table 1, entries V–XIII). In Fig. 4A, one can see an increase in α-helicity of the oligomers with increasing n via enhancement of the [θ]222 signal of the fractions of N-OK(Z) f12, f14, f15, f19 and f28 (Table 1, entries V–VII, IX, XIII) in TFE. Because of their low number of repeating units (n = 3–7), fractions of N-OK(TFA) f2, f3, f4 (Table 1, entries XVI–XIX) do not display helicity for f4, with only 19% helicity for f2. Therefore, as shown in Fig. 5, chain length dependence of α-helicity in TFE is demonstrated for the bis-functional fractionated samples with the Z-group protected moieties possessing low Đ values (<1.07), e.g. fractions of N-OK(Z): f28, f19, f15, f14, f12), indicating an almost linear increase in α-helicity (from 12% up to 33%) with increasing number of repeating units (n). It should be noted that this trend is also visible in the unfractionated samples: thus the unfractionated bis-functional oligomer N-OK(Z)-2, (n = 8) (Table 1, entry III) displays a lower α-helicity (18% in TFE) compared to the unfractionated bis-functional oligomer N-OK(Z)-3, (n = 24) (53% in TFE, 40% in HFIP) (Table 1, entry IV), yet confirming the increasing helicity behaviour of oligomers with increasing n as depicted with the “linear” line in Fig. 5.
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| Fig. 5 Depiction of increase in α-helicity [%] with respect to increasing number of repeating units (n) of fractions of N-OK(Z) in TFE (line is a guide for the eye only). | ||
The chain end effects introduced by alkyl groups on one end (mono-functional) e.g. OK(Z) and OK(TFA), or on both ends (bis-functional) e.g. N-OK(Z) and N-OK(TFA), of the oligomer chains were examined by CD spectroscopy in HFIP and in TFE (see Table 1). Mono-functional oligomers, OK(Z) (Table 1, entry I) and OK(TFA) (Table 1, entry XIV) with equal chain length show higher α-helicity in comparison to their bis-functional derivatives, N-OK(Z) (Table 1, entry II) and N-OK(TFA) (Table 1, entry XV), suggesting that the alkyl end groups do not favour the helix formation. Furthermore, side chain effects stemming from amino-protecting groups, Z(Cbz) and TFA on conformational changes were also studied. We found that there was no distinctive difference in their α-helicity values of N-OK(Z) and N-OK(TFA) oligomers induced by their side chains (Table 1, entries II and XV respectively). Thus for instance, fractions f19 (with Z) (entry IX, n = 6, 7) and f2 (with TFA) (entry XVI, n = 6 ± 1) possess similar α-helicity values. However, as shown in Table 1, there is a slight difference in α-helicity values for the fractions with lower n, e.g. f5 (entry XIX, n = 3–4) does not display α-helicity, whereas f25 (entry XII, n = 4 ± 1) and f28 (entry XIII, n = 3) with similar ns show 12% helicity in TFE.
From Table 1 it can be also seen that TFE promotes helicity38 compared to HFIP. Fraction f12 of N-OK(Z) (entry V) displays 32% α-helicity in TFE whereas only 19% α-helicity is observed in HFIP. In the case of the fractions of N-OK(Z) measured in TFE (entries V–XIII) α-helicity of more than 16% is observed with a number of repeating units higher than 8 (n > 8) starting from fractions f19 and f20 (entries IX and X respectively). TFE increases the stability and formation of the α-helices over HFIP, explained by comparing polarities of both solvents, where TFE is more polar than HFIP. Pengo and Pasquato et al.39 have indicated a correlation between the polarities of different solvents and the equilibrium of the formation of α-helix structures, proving that the more polar the solvent is e.g. TFE, the equilibrium shifts to the formation of α-helical structures, whereas the less polar solvents promote the formation of 310-helix structures. It has been stated that the hydroxyl group of TFE can bind to the carbonyl group in the peptide backbone via hydrogen bonding without disrupting the hydrogen bonding interactions between the carbonyls and the amines of the peptide forming the α-helical structure.40
Influence of solvent composition and effects of number of repeating units of the peptide on the dynamics of the secondary structure formation of peptides and PEG-peptide diblock copolymers have reported that α-helicity is increasing with increasing number of repeating units of a peptide chain and with addition of TFE.41,42
In our study the TEM images of the fractions of N-OK(Z), f19 and f28, obtained after preparation in TFE (c = 0.2 mg mL−1) are shown in Fig. 6. The end groups of both f19 and f28 are functionalized with two C11 vinyl chains. The repeating unit (n) of each sample is different; for f19, the repeating unit is n ≈ 7, indicating that helix formation is already favoured, whereas for f28 (n = 3) the α-helical turn could be only 1, stabilized only with the help of TFE solvent. The TEM image of f19 (n = 7) shows a dense mesh of large fibrils (see Fig. 6a), while stacks of fibrillar bundles are formed by f28 (n = 3) (see Fig. 6b).
As shown in Fig. 6, we chose fractions f19 and f28 to demonstrate the effect of number of repeating units (n), specifically in the case of very low Đ values, on the formation of fibrils due to their secondary structural interactions. We did also investigate fibril formation of various other samples (see Fig. 36S–40S†), where solvent of choice and the fraction between helical chain lengths have been probed. In addition to the data shown in Fig. 6 and the CD results discussed above (Table 1, Fig. 4 and 5), a higher propensity to form fibrils is accompanied with a higher degree to form alpha helices, suggesting the formed to be promoted by the latter. We propose that increasing α-helicity is crucial to form fibrils owing to their improved packing accompanied by a more precise conformational identity of the peptide with the lower entropy.
The so obtained data allow us to quantify the amount of secondary structure (α-helicity) present within the functionalized oligo-L-lysines of precise chain length on basis of eqn (1). It is crucial to understand peptide assemblies in view of the initial conformational interactions and their secondary structure formation, hence we here for the first time represent a rational approach to engineer future fibril forming systems, based on oligomeric-L-lysines with very low Đ values (Đ < 1.07). Last but not least, it should be also emphasized that such artificial fibril forming assemblies hold great potential applications as inhibitors for amyloidosis of complex proteins e.g. Aβ. The influence of lipidic alkyl end groups and chain length of peptide unit on the folding behaviours of peptides within a hybrid polymer can thus be quantified, prospectively reported in future work.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c9ra03099a |
| This journal is © The Royal Society of Chemistry 2019 |