Structural and conformational properties of (Z)-beta-(1-naphthyl)- dehydroalanine residue

To understand how chemical structure of beta-substituted alpha, beta-dehydroalanine (particularly size and pi conjugation of beta substituent) affects conformational property, x-ray crystallographic analysis was performed on Boc-Ala-Delta(Z) Nap-Val-OMe [Boc: t-butoxycarbonyl; Delta(Z) Nap: (Z)-beta-(1-naphthyl)dehydroalanine; OMe: methoxy] having the naphthyl group as a bulky beta substituent. Single crystals were grown by slow evaporation from an ethanol solution in the triclinic space group P1 with a = 9.528 (3) A, b = 12.410(4) A, c = 5.975(2) A, alpha = 96.77(3) degrees, beta = 102. 81(2) degrees, gamma = 88.74(3) degrees, V = 684.1(4) A3, and Z = 1. Phase determination was carried out by a direct method (SHELEXS), and the final structure was refined to R = 8.1% and R(w) = 9.0% for 1964 observed reflections. The bond lengths and bond angles of the Delta(Z)Nap residue, characterized by a sp(2) hybridized C(alpha) atom, did not differ from those of other dehydroresidues such as Delta(Z) Phe, Delta(Z) Leu, and DeltaVal essentially. The peptide backbone took a type II beta-turn conformation involving an intramolecular hydrogen bond between CO(Boc) and NH(Val), similar to di- or tripeptides containing a Delta(Z) Phe or Delta(Z) Leu residue in the second positions. Here the naphthyl group was found to be nonplanar [chi(2) = 55(1) degrees ] relative to the C(alpha)==C(beta)==C(gamma) plane. The nonplanarity was supported by conformational energy calculation. The molecular packing was stabilized by two kinds of intermolecular hydrogen bonds and van der Waals interactions. Naphthyl groups were arranged in a partially overlapped face-to-face orientation with a center-to-center distance of 5.97 A. For additional information, peptide Boc-(Ala-Delta(Z) Nap-Leu)(2)-OMe was synthesized and its solution conformation was investigated by (1)H-NMR spectroscopy. The hexapeptide showed the tendency to form a 3(10)-helical conformation in solution essentially. Conformational properties of Delta(Z) Nap residue, characterized by a type II beta-turn and 3(10)-helix, were supported by a conformational energy contour map of the Delta(Z)Nap residue.     

Long, chiral polypeptide 3(10)-helices at atomic resolution

The crystal-state preferred conformation of the terminally blocked hepta- and octapeptides with the general formula -(Aib)n L-Leu-(Aib)2- (n = 4 and 5, respectively), determined by X-ray diffraction, was found to be a right-handed 3(10)-helix stabilized by five and six consecutive intramolecular NH...O = C H-bonds of the C(10)-III type, respectively. The octapeptide structure represents the first observation at atomic resolution of a regular, chiral 3(10)-helix larger than two complete turns. In both cases the right handed screw sense of the helix is dictated by the presence of the single, internal L-residue. This study confirms the propensity of short peptides rich in Aib, the prototype of the amino acid residues dialkylated at the alpha carbon, to adopt a 3(10)-helical structure and is expected to help our understanding of the conformational preferences of the membrane-active, channel-forming, ion-transporting peptaibol antibiotics.     

Crystal structure of achiral nonapeptide Boc-(Aib-DeltaZPhe)4-Aib-OMe at atomic resolution: evidence for a 3(10)-helix

An x-ray crystallographic analysis was carried out for Boc-(Aib-DeltaZPhe)4-Aib-OMe (1: Boc = t-butoxycarbonyl; Aib = alpha-aminoisobutyric acid; DeltaZPhe = Z-alpha,beta-didehydrophenylalanine) to provide the precise conformational parameters of the octapeptide segment -(Aib-DeltaZPhe)4-. Peptide 1 adopted a typical 3(10)-helical conformation characterized by = +/-55.8 degrees (50 degrees -65 degrees), = +/-26.7 degrees (15 degrees -45 degrees), and = +/-179.5 degrees (168 degrees -188 degrees) for the average values of the -(Aib-DeltaZPhe)4- segment (the range of the eight values). The 3(10)-helix contains 3.1 residues per turn, being close to the "perfect 3(10)-helix" characterized by 3.0 residues per turn. NMR and Fourier transform infrared (FTIR) spectroscopy revealed that the 3(10)-helical conformation at the atomic resolution is essentially maintained in solution. Energy minimization of peptide 1 by semiempirical molecular orbital calculation converged to a 3(10)-helical conformation similar to the x-ray crystallographic 3(10)-helix. The preference for a 3(10)-helix in the -(Aib-DeltaZPhe)4- segment is ascribed to strong inducers of the 3(10)-helix inherent in Aib and DeltaZPhe residues-in particular, the Aib residues tend to stabilize a 3(10)-helix more effectively. Therefore, the -(Aib-DeltaZPhe)4- segment is useful to rationally design an optically inactive 3(10)-helical backbone, which will be of great importance to provide novel insights into noncovalent and covalent chiral interactions of a helical peptide with a chiral molecule.     

Conformational studies of Aib-rich peptides containing lactam-bridged side chains: evidence of 3(10)-helix formation

Aib-rich side-chain lactam-bridged oligomers Ac-(Glu-Aib-Aib-Lys)n-Ala-OH with n = 1,2,3 were designed and synthesized as putative models of the 3(10)-helix. The lactam bridge between the side chains of L-Glu and L-Lys in (i)--(i + 3) positions was introduced in order to enhance the structural preference toward the right-handed 3(10)-helix. The conformational properties of the three peptides were studied in trifluoroethanol (TFE) solution by CD, NMR, and computer simulations. The structural information was derived mainly from the analysis of nuclear Overhauser effect spectroscopy spectra. The presence of alpha H(i)-HN(i + 2) and of alpha H(i)-HN(i + 3) connectivities and the absence of alpha H(i)-HN(i + 4) connectivities indicate that these peptides fold into a 3(10)-helix rather than into an alpha-helix. Based on these conformational features, stereospecific assignment of the Aib methyl groups was possible. The results of such experiments and of the subsequent distance geometry and restrained molecular dynamics simulations reveal a marked preference of these peptides for 3(10)-helix. The CD spectra of these peptides indicate that the helix content increases upon chain elongation. The CD spectrum of the trimer is characterized by a negative band at 200 nm and by a weak positive band around 220 nm. The CD spectrum in TFE is different from that observed in aqueous solution in the presence of SDS micelles, reported in our previous work, and from those reported by a different research group for 3(10)-helical peptides. A possible reason for these differences could rest in the presence of different equilibria of the conformer populations of the various peptides in different solvent systems.     

Addition of side-chain interactions to 3(10)-helix/coil and alpha-helix/3(10)-helix/coil theory.

An increasing number of experimental and theoretical studies have demonstrated the importance of the 3(10)-helix/ alpha-helix/coil equilibrium for the structure and folding of peptides and proteins. One way to perturb this equilibrium is to introduce side-chain interactions that stabilize or destabilize one helix. For example, an attractive i, i + 4 interaction, present only in the alpha-helix, will favor the alpha-helix over 3(10), while an i, i + 4 repulsion will favor the 3(10)-helix over alpha. To quantify the 3(10)/alpha/coil equilibrium, it is essential to use a helix/coil theory that considers the stability of every possible conformation of a peptide. We have previously developed models for the 3(10)-helix/coil and 3(10)-helix/alpha-helix/ coil equilibria. Here we extend this work by adding i, i + 3 and i, i + 4 side-chain interaction energies to the models. The theory is based on classifying residues into alpha-helical, 3(10)-helical, or nonhelical (coil) conformations. Statistical weights are assigned to residues in a helical conformation with an associated helical hydrogen bond, a helical conformation with no hydrogen bond, an N-cap position, a C-cap position, or the reference coil conformation plus i, i + 3 and i, i + 4 side-chain interactions. This work may provide a framework for quantitatively rationalizing experimental work on isolated 3(10)-helices and mixed 3(10)-/alpha-helices and for predicting the locations and stabilities of these structures in peptides and proteins. We conclude that strong i, i + 4 side-chain interactions favor alpha-helix formation, while the 3(10)-helix population is maximized when weaker i, i + 4 side-chain interactions are present.     

Critical Main-Chain Length for Conformational Conversion From 3(10)-Helix to α-Helix in Polypeptides

To assess the minimal peptide length required for the stabilization of the alpha-helix relative to the 3(10)-helix in Aib-rich peptides, we have solved the X-ray diffraction structures of the terminally blocked sequential hexa- and octapeptides with the general formula-(Aib-L-Ala)n-(n = 3 and 4, respectively). The hexapeptide molecules are completely 3(10)-helical with four 1----4 intramolecular N-H . . . O = C H-bonds. On the other hand, the octapeptide molecules are essentially alpha-helical with four 1----5 H-bonds; however, the helix is elongated at the N-terminus, with two 1----4 H-bonds, giving these molecules a mixed alpha/3(10)-helical character. In both compounds the right-handed screw sense of the helix is dictated by the presence of the Ala residues of L-configuration. This study represents the first experimental proof for a 3(10)----alpha-helix conversion in the crystal state induced by peptide backbone lengthening only.     

External chirality-triggered helicity control promoted by introducing a beta-Ala residue into the N-terminus of chiral peptides

The noncovalent chiral domino effect (NCDE), defined as chiral interaction upon an N-terminus of a 3(10)-helical peptide, will provide a unique method for structural control of a peptide helix through the use of external chirality. On the other hand, the NCDE has not been considered to be effective for the helicity control of peptides strongly favoring a one-handed screw sense. We here aim to promote the NCDE on peptide helicity using two types of nonapeptides: H-beta-Ala-Delta(Z)Phe-Aib-Delta(Z)Phe-X-(Delta(Z)Phe-Aib)(2)-OCH(3) [Delta(Z)Phe = alpha,beta-didehydrophenylalanine, Aib = alpha-aminoisobutyric acid], where X as the single chirality is L-leucine (1) or L-phenylalanine (2). NMR, IR, and CD spectroscopy as well as energy calculation revealed that both peptides alone form a right-handed 3(10)-helix. The original CD amplitudes or signs in chloroform, irrespective of a strong screw-sense preference in the central chirality, responded sensitively to external chiral information. Namely added Boc-L-amino acid stabilized the original right-handed helix, while the corresponding d-isomer destabilized it or transformed it into a left-handed helix. These peptides were also shown to bind more favorably to an L-isomer from the racemate. Although similar helicity control was observed for analogous nonapeptides bearing an N-terminal Aib residue (Inai, Y.; et al. Biomacromolecules 2003, 4, 122), the present findings demonstrate that the N-terminal replacement by the beta-Ala residue significantly improves the previous NCDE to achieve more effective control of helicity. Semiempirical molecular orbital calculations on complexation of peptide 2 with Boc-(L or D)-Pro-OH reasonably explained the unique conformational change induced by external chirality.     

Raman spectra of copoly(D,L-alanines)

Raman spectra in the region 1000–150 cm^?1 were measured for copoly(D ,L -alanines) with the D -residue contents, 3, 7, 10, and 20%, and compared with the spectrum of the α-helical poly-L -alanine. The 532- and 378-cm^?1 peaks were assigned to the L -residues with a right-handed α-helix-like local conformation or to the D -residues with a left-handed α-helix-like local conformation. From the intensity of the latter peak the contents of these local conformations were estimated as a function of the D -residue contents for the copolymers. The 264-cm^?1 peak, which has been assigned to the breathing vibration of the α-helical poly-L -alanine, shows a marked decrease in its intensity upon the introduction of the D residues. This result suggests that the overall deformation vibration of the α-helix arises from rather long sequences of the L - and D -alanine residues with the α-helical conformation and that the intensity of this vibration depends on the content of these sequences in the copolymers.     

Design of peptides with alpha,beta-dehydro-residues: synthesis, and crystal and molecular structure of a 3(10)-helical tetrapeptide Boc-L-Val-deltaPhe-deltaPhe-L-Ile-OCH3.

The peptide Boc-L-Val-deltaPhe-deltaPhe-L-Ile-OCH3 was synthesized using the azlactone method in the solution phase, and its crystal and molecular structures were determined by X-ray diffraction. Single crystals were grown by slow evaporation from solution in methanol at 25 degrees C. The crystals belong to an orthorhombic space group P2(1)2(1)2(1) with a = 12.882(7) A, b = 15.430(5) A, c = 18.330(5) A and Z = 4. The structure was determined by direct methods and refined by a least-squares procedure to an R-value of 0.073. The peptide adopts a right-handed 3(10)-helical conformation with backbone torsion angles: phi1 = 56.0(6)degrees, psi1 = -38.0(6)degrees, phi2 = -53.8(6)degrees, psi2 = 23.6(6)degrees, phi3 = -82.9(6)degrees, psi3 = -10.6(7)degrees, phi4 = 124.9(5)degrees. All the peptide bonds are trans. The conformation is stabilized by intramolecular 4-->1 hydrogen bonds involving Boc carbonyl oxygen and NH of deltaPhe3 and CO of Val1 and NH of Ile4. It is noteworthy that the two other chemically very similar peptides: Boc-Val-deltaPhe-deltaPhe-Ala-OCH3 (i) and Boc-Val-deltaPhe-deltaPhe-Val-OCH3 (ii) with differences only at the fourth position have been found to adopt folded conformations with two overlapping beta-turns of types II and III', respectively, whereas the present peptide adopts two overlapping beta-turns of type III. Thus the introduction of Ile at fourth position in a sequence Val-deltaPhe-deltaPhe-X results in the formation of a 3(10)-helix. The crystal structure is stabilized by intermolecular hydrogen bonds involving NH of Val1 and carbonyl oxygen of a symmetry related (-x, y - 1/2, 1/2 + z) deltaPhe2 and NH of deltaPhe2 with carbonyl oxygen of a symmetry related (x, y1/2, 1/2 + z) Ile4. This gives rise to long columns of helical molecules linked head to tail running along [010] direction.     

Chiral interaction in Gly-capped N-terminal motif of 3(10)-helix and domino-type induction in helix sense

Chiral interaction of helical peptide with chiral molecule, and concomitant induction in its helix sense have been demonstrated in optically inactive nonapeptide (1) possessing Gly at its N-terminus: H-Gly-(Delta(Z)Phe-Aib)(4)-OCH(3) (1: Delta(Z)Phe = Z-dehydrophenylalanine; Aib = alpha-aminoisobutyric acid). Spectroscopic measurements [mainly nuclear magnetic resonance (NMR) and circular diochroism (CD)] as well as theoretical simulation have been carried out for that purpose. Peptide 1 in the 3(10)-helix tends to adopt preferentially a right-handed screw sense by chiral Boc-L-amino acid (Boc: t-butoxycarbonyl). Induction in the helix sense through the noncovalent chiral domino effect should be derived primarily from the complex supported by the three-point coordination on the N-terminal sequence. Thus the 3(10)-helical terminus consisting of only alpha-amino acid residues enables chiral recognition of the Boc-amino acid molecule, leading to modulation of the original chain asymmetry. Dynamics in the helix-sense induction also have been discussed on the basis of a low-temperature NMR study. Furthermore, the inversion of induced helix sense has been achieved through solvent effects.     

Peptide helices with pendant cycloalkane rings. Characterization of conformations of 1-aminocyclooctane-1-carboxylic acid (Ac8c) residues in peptides.

A pentapeptide, Boc-Leu-Ac8c-Ala-Leu-Ac8c-OMe 1, an octapeptide, Boc-Leu-Ac8c-Ala-Leu-Ac8c-Ala-Leu-Ac8c-OMe 2 and a tripeptide, Boc-Aib-Ac8c-Aib-OMe 3 containing the 1-aminocyclooctane-1-carboxylic acid residue (Ac8c) were synthesized and conformationally characterized by x-ray diffraction studies in the crystal state. Peptides 1 and 2 were also studied by NMR in CDC13 solution. Peptide 1 adopts a purely 3(10)-helical conformation in crystals, stabilized by three intramolecular 1 <-- 4 hydrogen bonds. Peptide 2 in crystals is largely 3(10)-helical with distortion in the backbone at the N-terminus by the insertion of a water molecule between Ac8c (2) CO and Ala (6) NH groups. Peptide 3 forms a C10-ring structure, i.e. a type III (III') beta- turn conformation stabilized by an intramolecular 1 <-- 4 hydrogen bond. Five cyclooctane rings assume boat-chair conformations, whereas the sixth [Ac8c(8) in 2] is appreciably distorted, resembling a chiral intermediate in the pseudorotational pathway from the boat-chair to the twisted boat-chair conformation. Internal bond angles of the cyclooctane rings are appreciably distorted from the tetrahedral value, a characteristic feature of the cyclooctane ring. Peptide 1 crystallized in the space group P212121 with a = 11.900(4) A, b = 18.728(6) A, c = 20.471(3) A and Z = 4. The final R1 and wR2 values are 0.0753 and 0.2107, respectively, for 3901 observed reflections [Fo > or = 3 sigma (Fo)]. Peptide 2 crystallized in space group P21 with a = 12.961(5) A, b = 17.710(10) A, c = 15.101(7) A, beta = 108.45(4) degrees and Z = 2. The final R1 and wR2 values are 0.0906 and 0.1832, respectively, for 2743 observed reflections [Fo > or = 3sigma (Fo)]. 1H-NMR studies on both the peptides strongly suggest the persistence of 3(10)-helical conformations in solution. Peptide 3 crystallized in the space group P21/n, with a = 10.018(1) A, b = 20.725(1) A, c = 12.915(1) A and Z = 4. The final R1 and wR2 values are 0.0411 and 0.1105, respectively, for 3634 observed reflections [Fo > or = 4sigma (Fo)].     

Structural features of linear, homo-Aib-based peptides in solution: a spectroscopic and molecular mechanics investigation.

In continuation of our studies on the determination of the structural features of functionalized peptides in solution by combining time-resolved fluorescence data and molecular mechanics results, the conformational properties of a series of linear, homo-Aib peptides in methanol (a structure-supporting solvent) were investigated. These compounds have the general formula P(Aib)nN, where Aib is alpha-aminoisobutyric acid, N is naphthalene and P is the monomethylated protoporphyrin IX, the two latter chromophores being covalently attached to the peptide C- and N-termini, respectively, while n=3, 6 and 9. According to 1H NMR and IR spectra, the peptides investigated largely populate a 3(10)-helical structure in CDCl3, which is also a structure-supporting solvent. Both steady-state and time-resolved fluorescence measurements show a strong quenching of the N emission that parallels an increase of the P fluorescence intensity, suggesting the occurrence of long-range energy transfer from 1N* to ground-state P. Comparison of quenching efficiencies and lifetime pre-exponents with those obtained theoretically from the deepest energy minimum conformers is very satisfactory. The computed structures, built up by partially taking into account the solvent medium, exhibit a rigid, highly compact arrangement, owing to both the 3(10)-helix conformation of the backbone chain and the very few peptide-to-chromophore covalent linkages. As a result, only one or two stable conformations for each peptide were theoretically found, in full agreement with the time-resolved fluorescence data. Orientational effects between the probes must be taken into account for a correct interpretation of the fluorescence decay results, which implies that interconversion among conformational substates of the N linkages is slower than 10 ns, corresponding to the upper limit of the energy transfer characteristic time.     

Critical Main-Chain Length for Conformational Conversion From 310-Helix to α-Helix in Polypeptides

Abstract

To assess the minimal peptide length required for the stabilization of the a-helix relative to the 3₁₀-helix in Aib-rich peptides, we have solved the X-ray diffraction structures of the terminally blocked sequential hexa- and octapeptides with the general formula -(Aib-L-Ala)_n-(n = 3 and 4, respectively). The hexapeptide molecules are completely 3₁₀-helical with four 1 ← 4 intramolecular N-H … O=C H-bonds. On the other hand, the octapeptide molecules are essentially α-helical with four 1 ← 5 H-bonds; however, the helix is elongated at the N-terminus, with two 1 ← 4 H-bonds, giving these molecules a mixed α/3₁₀-helical character. In both compounds the right-handed screw sense of the helix is dictated by the presence of the Ala residues of L-configuration. This study represents the first experimental proof for a 3₁₀ →α-helix conversion in the crystal state induced by peptide backbone lengthening only.     

Discriminating 3(10)- from alpha-helices: vibrational and electronic CD and IR absorption study of related Aib-containing oligopeptides

Model peptides based on -(Aib-Ala)(n)-, and (Aib)(n)-Leu-(Aib)(2) sequences, which have varying amounts of 3(10)-helical character, were studied by use of vibrational and electronic circular dichroism (VCD and ECD) and Fourier transform infrared (FTIR) absorption spectroscopies to test the correlation of spectral response and conformation. The data indicate that these peptides, starting from a length of about four to six residues, predominantly adopt a 3(10)-helical conformation at room temperature. The longest model peptides, depending on the series, may evidence some alpha-helical contribution to the spectra, while the shorter ones, with less than six residues, have much less order. The IR absorption spectra (as supported by theory) showed only small frequency changes between 3(10)- and alpha-helices. By contrast, solvent effects are a source of much bigger perturbations. The ECD results show that the intensity ratio for the approximately 222-nm to approximately 208-nm bands, while useful for distinguishing between these two helical types in some sequences, may have a narrower range of application than VCD. However, the VCD data presented here continue to support the proposed discrimination between alpha- and 3(10)-helices based on qualitative amide I and II bandshape differences. The present study shows the intensities of the 3(10)-helical amide I (peak-to-peak) to its amide II VCD to be of the same order and useful for discriminating them from alpha-helices, whose amide I dominates the amide II in intensity. This qualitative result is experimentally independent of the amount of alphaMe-substituted residues in the sequence. These experimental VCD results are consistent in detail with theoretical spectral simulations for Ac-(Ala)(8)-NH(2), Ac-(Aib-Ala)(4)-NH(2), and Ac-(Aib)(8)-NH(2) in 3(10)- and alpha-helical conformations.     

Variants of 3(10)-helices in proteins

An analysis of the shortest 3(10)-helices, containing three helical residues and two flanking capping residues that participate in two consecutive i + 3 --> i hydrogen bonds, shows that not all helices belong to the classic 3(10)-helix, where the three central residues adopt the right-handed helical conformation (alpha(R)). Three variants identified are: 3L10-helix with all residues in the left-handed helical region (alpha(L)), 3EL10-helix where the first residue is in the extended region followed by two residues in the alpha(L) conformation, and its mirror-image, the 3E'R10-helix. In the context of these helices, as well as the equivalent variants of alpha-helices, the length dependence of the handedness of secondary structures in protein structure is discussed. There are considerable differences in the amino acid preferences at different positions in the various types of 3(10)-helices. Each type of 3(10)-helix can be thought to be made up of an extension of a particular type of beta-turn (made up of residues i to i + 3) such that the (i + 3)th residue assumes the same conformation as the preceding residue. Distinct residue preferences at i and i + 3 positions seem to decide whether a particular stretch of four residues will be a beta-turn or a 3(10)-helix in the folded structure.     

A spectroscopic and molecular mechanics investigation on a series of AIB-based linear peptides and a peptide template, both containing tryptophan and a nitroxide derivative as probes

Linear Aib-based hexapeptides, of the general formula Ac-Toac-(Aib)(n) -Trp-(Aib)(r) -OtBu [T(Aib)(n) Trp], where n + r = 4, and Toac is a nitroxide spin-labeled C(alpha,alpha)-disubstituted glycine, were investigated by steady-state and time-resolved fluorescence measurements in different solvent media. A related peptide, i.e., cyclo-?Orn-[(Aib)(2)-Trp-(Aib)(2)-Z]-Asp-[(Aib)(2)-Toac-(Aib)(2)-+ ++OtBu ]? [T-cyclo-Trp], was also studied by the same techniques. It is a L-Orn, L-Asp diketopiperazine template, to which two Aib-based chains are covalently attached, each one containing one chromophore only, i.e., Trp or Toac. Whatever the solvent, in the former series of peptides quenching of the excited Trp exhibits three lifetime components and proceeds on a time scale from subnanoseconds to a few nanoseconds, while in the case of the template the same process occurs entirely on the nanoscale time scale, exhibiting two lifetimes only. The ir absorption spectral patterns suggest that the backbone of the peptides examined is in the 3(10)-helical conformation, as earlier determined by x-ray diffraction for T(Aib)(3)Trp in the crystal state. In all cases, the fluorescence results are satisfactorily described by a dipole-dipole interaction mechanism, in which electronic energy transfer takes place from the excited Trp to Toac, provided the mutual orientation between the fluorophore and Toac is taken into account. This implies that interconversion among conformational substates is slow on the time scale of the transfer process, allowing us to estimate the dynamics of the process. Molecular mechanics calculations coupled with time decay data made it possible to build up the most probable structures of these peptides in solution.     

Structural features of linear (alphaMe)Val-based peptides in solution by photophysical and theoretical conformational studies

In continuation of our studies on the determination of the structural features of functionalized peptides in solution by combining time-resolved fluorescence data and molecular mechanics results, the conformational features of a series of linear, L-(alphaMe)Val-based peptides have been investigated in methanol. These foldamers have the general formula F[(alphaMe)Val](r)-T-[(alphaMe)Val](2)NHtBu, where (alphaMe)Val = C(alpha)-methylvaline and r = 0-3, while F [= fluoren-9-ylmethoxycarbonyl (Fmoc)] and T [= 2,2,6,6-tetramethylpiperidine-1-oxyl-4-amino-carboxylic (Toac)] are a fluorophoric N(alpha)-protecting group and a nitroxide-based alpha-amino acid quencher, respectively. According to ir and CD spectra, the longest term of the series (r = 3) attains a 3(10)-helical structure, while the other peptides populate an intramolecularly H-bonded, 3(10)-helix-like conformation affected by dynamic helical distortions, which are enhanced by the shortness of the backbone chain. Such distortions are reflected in both the energy of the stretching mode and the molar extinction coefficient of the H-bonded N-H groups, the former being higher and the latter smaller than those of a stable 3(10)-helix. Steady-state and time-resolved fluorescence measurements in methanol show a strong quenching of Fmoc by the Toac residue, located at different helix positions, depending on the r value. Comparison of quenching efficiencies and lifetime preexponents with those theoretically obtained from the deepest energy minimum conformers, assuming a F?rster mechanism, is satisfactory. The computed structures exhibit a rather compact arrangement, which accounts for the few sterically favored conformations for each peptide, in full agreement with the time-resolved fluorescence data. Orientational effects between the probes must be taken into account for a correct interpretation of the fluorescence decay results, implying that interconversion among conformational substates involving the probes is slower than the energy transfer rate.     

Noncovalent chiral domino effect on one-handed helix of nonapeptide containing a midpoint L-residue

We here clarify whether noncovalent chiral domino effect characterized by the terminal interaction of a helical peptide with a chiral small molecule can alter the helical stability of N-deprotected peptides containing an L-residue covalently incorporated into the inner position. Two nonapeptides consisting of the midpoint L-leucine (1) or L-phenylalanine (2) and the achiral helix-forming residues were employed. NMR and IR spectroscopy and energy calculation indicated that both peptides adopt a 3(10)-helical conformation in chloroform. They strongly preferred a right-handed screw sense because of the presence of the midpoint L-residue. These original right-handed screw senses were retained on addition of chiral Boc-amino acid, but their helical stabilities clearly depended on its added chirality. Here, Boc-L-amino acid stabilizes the original right-handed helix, whereas the corresponding Boc-D-amino acid tends to less stabilize or destabilize it. This tendency was not observed for the corresponding N-Boc-protected peptides 1 and 2, strongly suggesting that the N-terminal amino group is required for controlling the stabilization of the original right-handed helix. Therefore, noncovalent chiral domino effect in peptides 1 and 2 can contribute even to the helical stability of a chiral peptide prevailing one-handed helix strongly through the midpoint L-residue. In addition, the N-terminal moiety of a 3(10)-helical peptide was found to generate chiral discrimination in complexation process with racemic additives.     

Structural features of model glycopeptides in solution and in membrane phase: a spectroscopic and molecular mechanics investigation

Model glycopeptides of the general formula Boc-Ala-Thr(G-D)-A(1)-A(2)-Leu-Leu-Lys(N)-Ala-OMe, where D = dansyl (dimethyl aminonaphthalenesulphonyl), G = glucosyl and N = naphthyl, while A(1)-A(2) = Ala-Leu or Aib-Aib, and denoted as D-G-Ala-N and D-G-Aib-N, respectively, were used to investigate glycoprotein-membrane interactions. They carry two fluorophores (D and N), covalently linked to the glucose ring and the lysine side chain, respectively, while the threonine side chain is O-glycosylated. CD spectra in different solvent media suggest that both glycopeptides attain an ordered structure, possibly a helix-like conformation. By combining FRET (fluorescence resonance energy transfer) experiments with molecular mechanics data, the most probable structures of both glycopeptides were built up, starting from both a right-handed (rh) alpha- and 3(10)-helix. They were found to populate an alpha-helical conformation, a result further confirmed by the very good agreement between theoretical and experimental quenching efficiency only observed when the backbone chain was in alpha-helix. The association of D-G-Ala-N with model membranes (liposomes) was studied by CD, fluorescence decay, fluorescence anisotropy, and collisional quenching experiments. The binding does not alter the structural features of the peptide because the CD spectral patterns are unaffected by the association. The peptide orientation inside the phospholipidic bilayer is guided by the polar glucose molecule lying in the water phase. The insertion of the hydrophobic backbone chain into the membrane, seeing the probes only partially accessible from the external solution, is characterized by a significant degree of heterogeneity, an increase in vesicles size, and a relevant stabilizing effect on the membrane itself against rupture by methanol.     

Studies of peptides forming 3(10)- and alpha-helices and beta-bend ribbon structures in organic solution and in model biomembranes by Fourier transform infrared spectroscopy

In order to examine the potential correlation between infrared absorption spectra and 3(10)- and alpha-helices and beta-bend ribbon structures, the secondary structures of synthetic peptides known to contain pure 3(10)-helices, mixed 3(10)/alpha-helices, and pure beta-bend ribbon structures, based upon X-ray diffraction and NMR studies, have been investigated by using FTIR spectroscopy incorporating resolution-enhancement techniques. Studies of the peptides known to contain a stable 3(10)-helix in CDCl3 show the main amide I band of fully stable 3(10)-helices occurs at 1666-1662 cm-1. Resolution-enhancement methods revealed small contributions at 1681-1678 and 1646-1644 cm-1, while the amide II band occurs at 1533-1531 cm-1. Peptides known to contain both alpha- and 3(10)-helices in their structure exhibit bands characteristic of both types of conformation. Peptides known to fold into the beta-bend ribbon structure show an amide I band maximum at 1648-1645 cm-1 with the amide II band at 1538-1536 cm-1. Incorporation of these peptides into model membrane structures, e.g., DMPC vesicles, in aqueous buffer sometimes produces changes in the peptide secondary structure. Those peptides which possess a 3(10)-helical structure in CDCl3 solution change the secondary structure in DMPC vesicles to predominantly alpha-helical, plus a contribution from short, unstable 3(10)-helix and/or beta-turns. Those peptides which contain a combination of alpha- and 3(10)-helical structures in CDCl3 solution tend to retain some 3(10)-helical structure within the lipid environment, although the overall H-bonding pattern is altered. Those peptides which form a beta-bend ribbon structure appear to be largely unaffected in the membrane environment.(ABSTRACT TRUNCATED AT 250 WORDS)