Fatemeh M.
Mir‡
a,
Marco
Crisma‡
b,
Claudio
Toniolo‡
b and
William D.
Lubell‡
*a
aDépartement de Chimie, Université de Montréal, C. P. 6128, Succursale Centre-Ville, Montréal, Québec, Canada H3C 3J7. E-mail: william.lubell@umontreal.ca
bDepartment of Chemistry, University of Padova and Institute of Biomolecular Chemistry, Padova Unit, CNR, 35131 Padova, Italy
First published on 10th June 2019
The unique abilities of homo-oligo-adamantyl peptides to adopt α- and γ-turn conformations are demonstrated by X-ray diffraction, and NMR and FT-IR absorption spectroscopies. Assembled by an Ugi multiple component reaction strategy, Nα-formyl-adamantyl tripeptide iso-propyl and tert-butyl amides are respectively found to adopt an isolated α-turn and an incipient γ-helix conformation by X-ray diffraction crystallography. The shortest example of a single α-turn with ideal geometry is observed in the crystalline state. In solution both peptides predominantly assume γ-helical structures.
Cα,α-Disubstituted glycines are known to be able to constrain peptides to adopt distinct secondary structures.6,7 The backbone ϕ and ψ torsion angles adopted by these residues are typically contingent on the substituent size and nature. Specifically, Cα,α-dimethylglycine (α-aminoisobutyric acid, Aib) and Cα-methylated analogs of proteinogenic amino acids favor folded backbone conformations in the 310-/α-helical region (ϕ = ±60 ± 20°, ψ = ±30 ± 20°),6,8,9 which are similarly adopted by peptides composed of 1-aminocycloalkane-1-carboxylic acid residues with four or more carbon atoms in the ring moiety.6b,7,9 Homo-peptides from the aforementioned residues almost invariably give rise to 310-helices,6b and only exceptionally to α-helices.10 These conclusions have been corroborated by a crystal-state investigation on a peptide featuring a single guest Gly residue placed in the middle of a host (Aib)16 homo-oligomer.11 On the other hand, a few highly sterically hindered residues, including 2-aminoadamantane-2-carboxylic acid (Adm) have been shown by X-ray diffraction analyses on model peptides to exhibit propensity for γ-turn conformations.5b,12,13 Finally, residues with two ethyl, n-propyl, phenyl or benzyl substituents adopt predominantly fully-extended (C5) conformations (ϕ ≅ 180°, ψ ≅ 180°).6b,7,14
Although homo-oligomers of Aib have been commonly prepared and studied,6,8 few examples of long oligopeptides composed of multiple residues with larger side chains have been reported due to the challenge of coupling sterically bulky α-amino acids, particularly at their α-amino functionality.15 In this connection, it is worth pointing out that the sterically hindered Adm residue has been shown to react with protein amino acids (Gly, Leu, Phe) in acceptable yields (45–75%) by classical C-activating methods [i.e., Nα-unprotected N-carboxyanhydride, Nα-acetyl/trifluoroacetyl 5(4H)oxazolones and EDC (N-ethyl-N′-3-(dimethylaminopropyl)carbodiimide)/HOAt (7-aza-1-hydroxy-1,2,3-benzotriazole)] to provide simple dipeptides with N-terminal Adm residues.12,16 The synthesis of dipeptides with C-terminal Adm residues is however more challenging and has been achieved (65–90% yield) using reactive acyl chloride derivatives, combined usually with an azide (–N3) precursor of the α-amino group,12 according to the procedure of Meldal,17 but coupling yields drop precipitously (<10%) upon homo-peptide assembly to the tripeptide level, preventing further main-chain elongation.12
Among the potentially useful, alternative methods for synthesizing Cα,α-disubstituted glycines with very bulky side chains, the Ugi reactions of adamantan-2-one has previously delivered -Adm-Gly- dipeptides, albeit in modest yields.18a Furthermore, HCO-Aib-Aib-OMe [OMe, (methoxy)] has been assembled in 57% yield by the reaction of methyl 2-isocyano-2-methylpropanoate, acetone and ammonium formate.18b To the best of our knowledge, the construction of longer main chains of severely sterically bulky amino acids by the Ugi reaction has yet to be reported. Exploring the Ugi conditions, we present here access to the HCO-(Adm)3-NHR tripeptides 1 and 2 (R = iPr and tBu, respectively). A concomitant combination of X-ray diffraction crystallography and spectroscopic methods has demonstrated that the Adm residue can favor the elusive single 13-membered intramolecularly hydrogen-bonded α-turn, as well as the almost completely developed γ-helix conformations.
Entry | ϕ 1 | ψ 1 | ϕ 2 | ψ 2 | ϕ 3 | ψ 3 |
---|---|---|---|---|---|---|
1 From acetone | −52.4 | −49.0 | −59.3 | −46.5 | −59.7 | −59.6 |
1 From acetone/CHCl3 | −52.8 | −48.6 | −59.6 | −46.0 | −59.5 | −60.3 |
1 From acetone/EtOAc/CHCl3 | −52.8 | −48.8 | −59.5 | −46.0 | −59.6 | −60.2 |
2 From acetone/EtOAc | 82.1 | −84.1 | 74.3 | −82.3 | 80.3 | −113.2 |
In addition, the formamide carbonyl oxygen is at a distance of 3.117(3) Å from the nitrogen atom of Adm(3), suitable for forming a 10-membered intramolecular hydrogen bond (β-turn),19 but the H⋯O separation (2.61 Å) and N–H⋯O angle (117.4°) would be slightly outside the commonly accepted limits (≤2.50 Å and ≥ 120°) for the occurrence of a hydrogen bond.20 In the quest for possible polymorphs, peptide 1 was also crystallized from solvents of varying polarity (EtOAc, acetone, CHCl3) within the limits imposed by solubility. Crystals suitable for X-ray diffraction analysis were obtained from three different systems; however, all gave the identical α-turn structure, within experimental error (Table 1).
As stated above, crystallography of single α-turns is very unusual.4 In most of the examples, the backbone torsion angles are significantly distorted in comparison with those observed in regular α-helices. Conversely, in the crystal structure of 1, the average ϕ and ψ torsion angles over the three Adm residues (−57°, −52°) differ only by 6° and 10°, respectively, from the canonical values (−63°, −42°) based on statistical analysis of α-helices in crystalline peptides.2c To the best of our knowledge, the structure of 1 represents the shortest peptide sequence giving rise to an isolated α-turn of regular geometry.
In the X-ray diffraction structure of tripeptide 2, the backbone torsion angles (Table 1) and distances between hydrogen-bond donor and acceptor atoms demonstrate the presence of two consecutive γ-turns5b at the level of the Adm(1) and Adm(2) residues (Fig. 1b and ESI†). Two intramolecular hydrogen bonds are observed, namely between the formamide carbonyl oxygen and the NH group of Adm(2), and between the carbonyl oxygen of Adm(1) and the NH group of Adm(3). The former hydrogen bond is significantly elongated [N⋯O 3.1665(15) Å, H⋯O 2.572(18) Å, N–H⋯O angle 129.4(15)°] in comparison to the latter [N⋯O 2.8804(14) Å, H⋯O 2.31(2) Å, N–H⋯O angle 124.5(16)°]. Indeed, the backbone torsion angles of Adm(1) deviate more markedly than those of Adm(2) from the ideal values of a γ-turn structure (ϕ, ψ = 75°,−75°).5 The shorter intramolecular hydrogen bond may be due in part to London dispersion between the adamantane moieties of Adm residues 1 and 3;21 three H⋯H contacts (the shortest of which separated by 2.34 Å) are observed. The longer intramolecular hydrogen bond is associated with a 7.8° larger ϕ1 value, compared to that of ϕ2, in contrast to the less than 2° difference in the values of ψ1 and ψ2. The distortion of ϕ1 weakens the N2–H⋯O0 intramolecular hydrogen bond, but enables the N1–H group to participate in an intermolecular hydrogen bond with the O2 atom of a symmetry related molecule (ESI†). The torsion angles of Adm(3) fall also in the lower-right quadrant of the Ramachandran map as those of the two preceding residues, but formation of a third γ-turn is not observed. Conversely, the carbonyl oxygen of Adm(2), which could be the potential acceptor of the γ-turn hydrogen bond, is involved in an intermolecular hydrogen bond with the N1–H group of a symmetry-related molecule (ESI†), and the C-terminal amide NH group is not engaged in any hydrogen bond. To avoid intermolecular steric clashes in the crystal, the ψ torsion angle of Adm(3) is forced to adopt a value (−113.2°) which prevents the C-terminal amide NH group from approaching the carbonyl oxygen of Adm(2) at a suitable hydrogen-bond distance.
The calculated density for the crystals of 1 (1.254 g cm−3) was less than that of 2 (1.302 g cm−3). The packing mode of tripeptide 1 features one N–H⋯OC hydrogen bond, three C–H⋯O contacts within the distance of 2.66 Å,22 and four H⋯H contacts within van der Waals distance. In the packing mode of tripeptide 2, intermolecular interactions include one N–H⋯OC hydrogen bond, as well as two C–H⋯O contacts and nine aliphatic H⋯H contacts in the range 2.10–2.39 Å. Within the sum of the van der Waals radii, the latter may stabilize the packing and account for the higher density of crystals of 2 through London dispersion.21
Sequence assignments of the NH proton resonances in the NMR spectra of peptides 1 and 2 in CDCl3 were achieved by a combination of COSY and HMBC experiments, the latter optimized to identify long-range, through-bond J couplings (ESI†).
Solvent shielded and exposed NH protons were examined by studying influences of changes in environment on the chemical shifts of their signals (Table 2). Amide protons involved in hydrogen bonds display typically little variation in their chemical shifts upon changes in solvent composition and temperature.23 As for peptides 1 and 2, switching NMR solvent from CDCl3 to dimethylsulfoxide (DMSO, d6) caused significant (2.37 and 2.58 ppm, respectively) downfield shifts for only the formamide NH proton signal, suggesting that this group is exposed to solvent in contrast to the other NH proton signals which exhibited limited variations in chemical shifts (0.02 to 0.22 ppm). This different behavior of the formamide NH proton is already evident at the very beginning (2% DMSO in CDCl3) of the solvent titration curves (Fig. 2). Similarly, for both peptides 1 and 2, changes in temperature in the two solvents influenced significantly (Δδ/ΔK = −3.8 to −5.2 ppb K−1) the formamide NH signal relative to those of the other amide protons. The NH chemical shifts of the latter protons varied less with temperature in the solvent of lower polarity CDCl3 (Δδ/ΔK = −0.3 to −1.5 ppb) than in DMSO (Δδ/ΔK = −1.0 to −3.3 ppb K−1).
entry | δ CDCl3 | δ DMSO | Δδ/Δsol | Δδ/ΔK | Δδ/ΔK |
---|---|---|---|---|---|
CDCl3 | DMSO | ||||
1: R = iPr | |||||
1NH | 5.67 | 8.04 | 2.37 | −4.3 | −4.2 |
2NH | 7.17 | 7.37 | 0.20 | −0.3 | −1.2 |
3NH | 7.00 | 7.02 | 0.02 | −1.4 | −1.5 |
4NH | 7.02 | 7.18 | 0.16 | −1.3 | −3.3 |
2: R = tBu | |||||
1NH | 5.46 | 8.04 | 2.58 | −5.2 | −3.8 |
2NH | 7.16 | 7.38 | 0.22 | −0.3 | −1.1 |
3NH | 6.69 | 6.91 | 0.22 | −0.45 | −1.0 |
4NH | 7.07 | 7.05 | 0.02 | −1.5 | −2.5 |
Notably, an X-ray diffraction analysis of crystals of peptide 2 grown from DMSO (bis-DMSO solvate) highlighted the presence of only one γ-turn in each of the two independent but similar peptide conformers A and B in the crystal matrix (Fig. 3 and ESI†). The surviving intramolecular hydrogen bond occurred between the formamide carbonyl oxygen and the NH group of Adm(2). The sets of ϕ and ψ torsion angles of Adm(1) in the two peptide conformers were −75.4°, 74.8°, and 76.6°, −69.9°, respectively. Three intermolecular hydrogen bonds were observed between each peptide and two co-crystallized DMSO solvent molecules: one between the Adm(1) NH group and the oxygen atom of one molecule of DMSO, and the other two between the Adm(3) and tert-butyl amide NH groups together with the oxygen atom of a second DMSO molecule. In each peptide conformer, Adm(2) and Adm(3) were helical but of opposite screw sense: ϕ2, ψ2, ϕ3, ψ3 = 59.8°. 64.1°, −59.0°, −55.5° (in A); −60.0°, −66.9°, 61.1°, 58.5° (in B).
In the N–H stretching region (3500–3200 cm−1), the FT-IR absorption spectra of peptides 1 and 2 in CDCl3 solution (Fig. 4) are very similar, and characterized by a band at 3412–3414 cm−1 (free, solvated NH groups) accompanied by a much broader band with maximum near 3300 cm−1 (hydrogen-bonded NH groups).24 The latter band is significantly skewed to higher wavenumbers. For both compounds, no significant differences in spectral shape and in the relative intensity of the hydrogen-bonded versus free N–H stretching bands were found over the concentration range 10.0 mM–0.1 mM (ESI, Fig. S3 and S4†), suggesting strongly that the observed hydrogen bonding is essentially intramolecular. In addition, these curves do not provide any evidence for concentration-dependent conformational transitions. The solid-state FT-IR spectra of the crystals of peptides 1 and 2 have also been recorded (ESI, Fig. S5 and S6†). They are clearly different, particularly in the N–H stretching region. However, unambiguous dissection of contributions from inter- and intramolecular hydrogen bonds to the observed bands is problematic (in spite knowledge of hydrogen-bonding and related geometrical parameters from the X-ray crystal structures), thus hampering a meaningful correlation with the spectra in solution. Overall, the FT-IR spectra of both peptides in solution are compatible with the occurrence of multiple, more-or-less strongly hydrogen-bonded, γ-turns. Conversely, a prevailing population of a single α-turn or combinations of two β-turns or a β-turn encompassed within an α-turn, all are unlikely. These conformers, in which the ratio of free to hydrogen bonded NH groups would be respectively 3/1 and 2/2, would exhibit spectral shapes different from those reported in Fig. 4. Moreover, the maximum of the band associated with hydrogen-bonded N–H groups in α- or β-turns would be located at wavenumbers significantly higher than 3300 cm−1.24 Taken together, the observed NMR and FT-IR absorption data indicate that both peptides assume predominantly γ-helical structures in solution. The capabilities of these spectroscopic techniques are however unable to detect or rule out the presence of a concomitant small population of α-turn conformation.
Fig. 4 FT-IR absorption spectra (N–H stretching region) of HCO-(Adm)3-NHiPr (1) and HCO-(Adm)3-NHtBu (2) in CDCl3 solution. Peptide concentration: 1.0 mM. |
Considering the marginal role of the crystallization solvent properties to significantly bias the conformations of peptides 1 and 2, the chemical structure of the C-terminal substituent R (iPr or tBu) is likely responsible for the outcome in the crystal states (α-turn or γ-turn). An example has already been reported of two homo-peptides differing only in their C-terminal group (ethyl ester vs. tert-butyl ester) giving rise to two different conformations in the crystal state, but adopting apparently the same conformation in solution.14a,b In such cases, self-assembly processes leading to crystal nucleation may favor a minor conformer present in solution depending on the C-terminal group. Subsequently, crystal growth will be governed by the templating effect of the crystal nuclei. A synthetic and conformational study on a large set of appropriately designed model compounds is planned in our laboratories, aimed at further exploring the effect of the C-terminal substituent on the 3D-structure of Adm-based peptides.
Considering the power of the Ugi multiple component method reported in this work for synthesizing sterically hindered peptides, potential now exists to harness bulky residues for various studies in peptide science. The unique γ-helical folding pattern which was observed both in solution and in the crystal state, as well as the fascinating diamondoid hydrocarbon side chains may similarly lend themselves for novel applications. In this connection, adamantane-functionalized compounds [particularly its –NH- and –C(O)– derivatives] have already found important applications in medicinal chemistry as drugs to treat parkinsonism and related syndromes, and as antiviral agents to combat type-A influenza virus in humans.25 Moreover, growing interest for adamantane and related structures is currently being observed in other areas, including nanotechnology (as organic microelectronic components and coating agents), polymers, molecular recognition, and supramolecular chemistry.26
Footnotes |
† Electronic supplementary information (ESI) available: General information, experimental procedures, compounds characterization, crystallographic data, 1H, 13C and 2D NMR spectra, FT-IR absorption spectra. CCDC 1906513, 1906514, 1906515, 1906516 and 1906517. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c9sc01683j |
‡ The manuscript was written through contributions of all authors. The syntheses were all performed by FMMir. |
This journal is © The Royal Society of Chemistry 2019 |