Synthesis of oligopeptides consisting of L-leucyl-L-leucyl-L-ananyl and L-methionyl-L-methionyl-L-leucyl repeating units with an improved preparation of Nps-amino acids

Two series of peptides with hydrophobic side chains, Nps-(L -Leu-L -Leu-L -Ala)_n-OEt and Nps-(L -Met-L -Met-L Leu)_n-OEt (n = 1–6), were synthesized by the fragment condensation method using dicyclohexylcarbodiimide in the presence of N-hydroxysuccinimide. The tripeptide fragments were prepared stepwise by dicyclohexylcarbodiimide-mediated reaction of Nps-amino acids, which were synthesized by an improved rapid procedure.     

Unusual conformational transitions of leucine-containing basic polytripeptides

The conformational transitions of synthetic basic polytripeptides (Lys-Leu-Gly)_n, (A₂bu-Leu-Gly)_n, (Lys-Leu-Ala)_n, and (A₂bu-Leu-Ala)_n induced by high salt concentrations and elevated pH were investigated by CD, ir, and ¹H-nmr spectroscopy, sedimentation analysis, viscometry, and light scattering. Sheet aggregates of chains in a conformation similar to the polyglycine II (polyproline II) helix, bound together by hydrogen bonds, are the most probable form of (Lys-Leu-Gly)_n and also, partly, of (A₂bu-Leu-Gly)_n in a high-pH or high-salt solutions. The conformation (Lys-Leu-Ala)_n, in a low-salt concentration, is an α-helix. Since (A₂bu-Leu-Ala)_n is disordered under similar conditions, it appears that this α-helix is stabilized by hydrophobic interactions between Lys and Leu side chains. In a high concentration of water structure-making ions, CD data for (Lys-Leu-Ala)_n indicate distortion of the α-helix, with a parallel increase in the average molecular weight corresponding to trimer formation. Hydrodynamic data are consistent with a model of bundles of three closely touching spherocylinders. (A₂bu-Leu-Ala)_n shows a limited tendency to α-helix formation.     

Conformation of oligopeptides with L-leucyl-L-leucyl-L-alanyl and L-methionyl-L-methionyl-L-leucyl repeating units

The conformation of oligopeptides with hydrophobic side chains, Nps-(L -Leu-L -Leu-L -Ala)_n-OEt and Nps-(L -Met-L -Met-L -Leu)_n-OEt(n = 1–6), in the solid state, obtained either by evaporation of the solvent or by precipitation with diethyl ether from a 1,1,1,3,3,3-hexafluoropropan-2-ol (HFIP) solution, has been studied with ir spectroscopy and x-ray powder-diffraction measurements. The conformation of these peptides in the HFIP solution has been studied by CD spectroscopy. Due to a strong preference of the amino acids to form an α helix, the peptides begin forming α helices at the dodecapeptide in the HFIP solution, and in the solid state by evaporation. In the solid state, with precipitation, the α-helical conformation is first observed at the octadecapeptide and the lower peptides assume a β structure. The conformational change, from the α helix to the β structure of the peptides with 12 to 15 amino acid residues, during the precipitation process, is due to a strong tendency of the amino acids to form the β-structure in rather short peptide lengths.     

Vibrational analysis of peptides,polypeptides, and proteins. XVIII. Conformational sensitivity of the α-helix spectrum: αI- and αII-Poly(L-alanine)

The α_II-helix (? = ?70.47°, ψ = ?35.75°) is a structure having the same n and h as the (standard) α_I-helix (? = ?57.37°, ψ = ?47.49°). Its conformational angles are commonly found in proteins. Using an improved α-helix force field, we have compared the vibrational frequencies of these two structures. Despite the small conformational differences, there are significant predicted differences in frequencies, particularly in the amide A, amide I, and amide II bands, and in the conformation-sensitive region below 900 cm^?1. This analysis indicates that α_II-helices are likely to be present in bacteriorhodopsin [Krimm, S. & Dwivedi, A. M. (1982) Science 216 , 407–408].     

Vibrational circular dichroism of polypeptides. IV. Film studies of L-alanine homo-oligopeptides

Vibrational CD (VCD) and ir absorption data are reported for a series of films of Boc-(L -Ala)_n-OMe homo-oligopeptides (n = 3–7) in the amide I and A regions. The data evidenced a sharp change between n = 3 and n = 4, which parallels the onset of β-structure formation, and another between n = 5 and n = 6, which parallels the full development of β-structure. This represents the first report of the application of VCD to oligopeptide conformation. The data resembled earlier reported film VCD studies of higher-molecular-weight polypeptides of known β-structure.     

Basic polypeptides as histone models. Synthesis, conformation, and interaction with DNA of statistical copolymers (Lys x,Ala y)n.

Statistical copolymers (Lys^x,Ala^y)_n were synthesized by copolymerization of N-carboxyanhydrides of L -amino acids. The conformation of copolymers in aqueous solutions was investigated using circular dichroism (CD). Calculations based on the CD data showed that polymers (Lys^x,Ala^y)_n can exhibit a random conformation, an α-helix, and a β-structure in various ratios. CD spectra of complexes of copolymers with DNA prepared by gradual dialysis from a high ionic strength to 0.15 M NaCl can be correlated with the copolymer conformation in medium and high ionic strength. For copolymers forming an α-helix and β-structure, these spectra show resemblance with similar spectra of complexes of those histones that are able to exhibit ordered conformations.     

Vibrational circular dichroism spectra of three conformationally distinct states and an unordered state of poly(L-lysine) in deuterated aqueous solution

Fourier transform ir vibrational circular dichroism (VCD) spectra in the amide I′ region of poly(L-lysine) in D₂O solutions have confirmed the existence of three distinct conformational states and an unordered conformational state in this homopolypeptide. Characteristic VCD spectra are presented for the right-handed α-helix, the antiparallel β-sheet, an extended helix conformation previously referred to as the so-called “random coil,” and a completely unordered conformation characterized by the absence of any amide I′ VCD. VCD for the antiparallel β-sheet in solution and the unordered chain conformation are presented for the first time. Each of the four different VCD spectra is unique in appearance and lends weight to the view that VCD has the potential to become a sensitive new probe of the secondary structure of proteins in solution.     

Conformation of sequential and random lysine–phenylalanine copolypeptides

The sequential copolypeptides (Lys-Phe-Lys)_n and (Lys₂-Phe-Lys)_n and a series of related random copolypeptides were investigated with respect of their ability to adopt the α-helix or β-conformation. Conformational transitions were induced by increasing the pH or by addition of NaClO₄ or methanol and were observed by recording the CD spectra. In contrast to the respective alternating copolypeptide (Phe-Lys)_n with its strong tendency for the β-structure reported previously, (Lys-Phe-Lys)_n can adopt either secondary structure, whereas (Lys₂-Phe-Lys)_n strongly favors the α-helix. Together with the random copolypeptides, whose composition varied from 20 to 50 mol % phenylalanine and whose average molecular weights ranged from 10,000 to 90,000, the influence of the phenylalanine content and of the chain length on conformational stability and the rotatory strength of the respective secondary structures were elaborated.     

Vibrational circular dichroism of polypeptides. VI. Polytyrosine alpha-helical and random-coil results

We have measured the VCD of polytyrosine in the amide I and II regions in dimethyl sulfoxide (DMSO) and in 80:20 mixtures of DMSO with trifluoroethanol, trifluoroacetic acid (TFA), and dichloroacetic acid and in 50:50 mixtures of DMSO and trimethyl phosphate (TMP). Additionally, VCD was obtained for deuterated polytyrosine in DMSO and DMSO:D₂O, DMSO:TFA(d₁), and DMSO:TMP mixtures as before. Amide A VCD was obtained in DMSO and DMSO:TMP mixtures. In the pure solvent, VCD of an opposite sign was seen as compared with that seen in the mixtures. The latter were characteristic in sign pattern and shape of right-handed α-helices for poly(L -tyrosine). The pure polytyrosine:DMSO results are similar to those of polylysine:D₂O at neutral pH and poly(β-benzyl-aspartate) in DMSO and may be characteristic of random-coil VCD.     

Experimental study of the conformation of two stereoregular polymethionines: poly(D-methionyl-L-methionine) and poly(L-methionyl-D-methionyl-L-methionine) (author's transl)]

Infrared spectroscopy, X-ray diffraction, and nuclear magnetic resonance spectroscopy have been used in investigating the conformation of two stereoregular polymethionines, poly(D -methionyl-L -methionine) and poly(L -methionyl-D -methionyl-L -methionine). When dissolved in a helicogenic solvent, such as chloroform and hexafluoroisopropanol, the polytripeptide is in an α-helical conformation. A helix-to-coil transition can then be induced by addition of trifluoroacetic acid. On the other hand, it appears that the most stable conformation of poly(D -Met-L -Met) is a β antiparallel folded structure in which the linear polypeptide segments are near to the planar extension. This structure has been evidenced through X-ray examination of oriented films, casted from solutions in chloroform. It has also been identified in solution in the same solvent, by use of infrared spectroscopy and by measuring the δ_Hα chemical shift which characterizes the H^α proton in the peptide units. This δ_Hα value is found equal to 5.4 ppm and differs significantly from those which are usually attributed to the α-helical conformation (δ_Hα = 4.2 ppm) and to the random coil (δ_Hα = 4.6 ppm). The β folded conformation of the poly(D -Met-L -Met) appears to be comparatively less stable than the α-helical one for the poly(L -Met) macromolecular stereoisomer since hexafluoroisopropanol is a helicogenic solvent for this last solute and a destabilizing one for the poly(D -Met-L -Met) β folded conformer. X-ray examinations carried out with stretched films, casted from a solution of poly(D -Met-L -Met) in chloroform, result in several data concering the cross β structure of this stereoregular polypeptide in the solid state.     

Conformational studies on poly(N-δ-trimethyl-l-ornithine)

$\text{Poly}\text{(N-δ-}\text{trimethyl-}\text{l}\text{-ornithine}$), (Me₃Orn)_n, is usually not able to attain the α-helical conformation in aqueous solution independent of its pH value; however, it becomes α-helical at low concentrations of sodium perchlorate over a wide pH range according to the circular dichorism (c.d.) spectra. Cl^?, SO₄^2? and H₂PO₄^? do not induce α-helix formation. One can conclude that a distinct topology of the anions bound by the side chains is responsible for the α-helix-inducing effect of some water-structure-breaking anions such as perchlorate. This means that the anions are inserted between the ?N⁺ of the side groups shielding the positive charges repelling one another. The insertion of the anions requires that the water molecules surrounding the ions can be stripped off, which is easily possible if they are water-structure-breaking ones. At higher perchlorate concentrations, the c.d. spectrum changes. It is characterized by a negative shoulder near 208 nm and a pronounced minimum at ≈ 226 nm. With increasing temperature, the c.d. spectrum of the α-helix occurs. Finally the α-helix undergoes a conformational change to the random coil. The apparent transition enthalpy ΔH_vH is remarkably lower than that of the homologue (Me₃Lys)_n, obviously due to a lower cooperativity of the transition. In contrast to poly(l-ornithine), (Orn)_n, the c.d. spectrum of (Me₃Orn)_n remains almost unchanged after adding anionic surfactants such as sodium octyl sulphate (SOS) or sodium dodecyl sulphate (SDS). In organic solvents like methanol or isopropanol, in contrast to (Orn)_a and (Lys)_n, no α-helix formation occurs. However, in mixtures of these alcohols or dioxane with water, α-helix formation is induced by perchlorate, as in pure water. The thermal stability of the α-helix in these systems is increased.     

Conformational studies of polymers and copolymers of L-aspartate ester. II. Infrared studies and the factors involved in the formation of the omega-helix

It has already been show that the helix senses of poly(β-benzyl L -aspartate) and poly(β-methyl L -aspartate) are left-handed, while the poly esters of n-propyl, isopropyl, n-butyl, and phenethyl L -asparate are all right-handed. The effect of changes in helix sense from the left-handed to the right-handed α-helical form on the infrared spectra of copolymers of benzyl L -aspartate with ethyl, n-butyl, isopropyl, n-propyl, and phenethyl L -aspartate have been studied. Those show that for the right-handed helical form the amide band frequencies fall within the range given by Elliott,⁷ while for the left-handed form the frequencies are higher. The frequency ranges for the two helix senses are given and have been used to show that poly (β-n-propyl L -aspartate) in chloroform solution undergoes a transition from the right-handed to the left-handed helix form on heating. Polarized infrared studies of the different copolymers show that the disposition of the side chain ester groups is different for the two forms. Although methyl L -aspartate forms a left-handed α-helix similar to benzyl L -aspartate, the introduction of methyl L -aspartate residues into poly (β-benzyl L -aspartate) prevents the formation of the ω-helix. The factors involved in the formation of this helix form are discussed.     

Synthesis and conformational characterization in the solid state of peptides consisting of L-phenylalanyl-L-phenylalanylglycyl and L-phenylalanyl-L-leucylglycyl residues

Two series of peptides containing L -phenylalanine, Nps-(L -Phe-L -Phe-Gly)_n-OEt (n = 1–6) and Nps-(L -Phe-L -Leu-Gly)_n-OEt (n = 1–7), were prepared by the fragment-condensation method using the tripeptide N-hydroxysuccinimide esters. Conformational characterization of these peptides in the solid state was performed by ir spectroscopy and x-ray powder diffraction measurement. The peptides Nps-(L -Phe-L -Phe-Gly)_n-OEt take the β-structure, but the pentadecapeptide and higher peptides of Nps-(L -Phe-L -Leu-Gly)_n-OEt form the α-helix, although the lower homologs take the β-structure.     

Synthesis and conformation of a polyoxyethylene-bound undecapeptide of the alamethicin helix and (2-methylalanyl-L-alanine)1–7

The stepwise synthesis and conformational studies of the N-terminal helical partial sequence of the membrane-modifying polypeptide antibiotic alamethicin are described. The polyoxyethylen esters of the fragments N-t-Boc-L -Pro-Aib-Ala-Gln-Aib-Val-Aib-Gly-OH and N-Ac-Aib-L -Pro-Aib-Ala-Aib-Ala-Gln-Aib-Val-Aib-Gly-OH are synthesized using polyoxyethylene (molecular mass 10,000) as solubilizing support. CD spectra of each intermediate in ethanol show α-helix formation of the N-protected peptide polymers beginning with the nonapeptide and of the N-protonated sequences beginning with the decapeptide. Compared to the helix of alamethicin, temperature- and solvent-dependent CD measurements indicate analogous conformational behavior. The results suggest that in lipophilic media the alamethicin helix can extend the full length of the partial sequence between the two proline residues and that aqueous media favor an increase of random-coil conformation. For model studies of the particular lipid interaction of alamethicin, the stepwise synthesis of peptides with the alternating (Aib-L -Ala)_n sequence (n = 1–7) was carried out on a polyoxyethylene support (molecular mass 6000). CD and ORD studies in ethanol showed a change from the random coil to a right-handed α-helix with increasing peptide length. This change is observed for the N-protected peptides at a chain length of 8 residues and for the N-protonated peptides at a length of 9 residues. The comparison of the CD data of free and polyoxyethylene-bound peptides revealed that the solubilizing polymeric support cannot induce conformational changes. The intensities of the CD bands of t-Boc-(Aib-L -Ala)_n-OPOE (n ≥ 6) are higher than those of alamethicin, and these model peptides show similar temperature and solvent inducible changes of their helix contents.     

1H-nmr study of protected methionine homo-oligopeptides in helix-supporting environment

¹H-nmr spectra for a series of Boc-L -(Met)_n-OMe (n = 2–9) homo-oligopeptides have been observed in the helix-supporting solvent trifluoroethanol (TFE) at millimolar concentrations. Interfering solvent peaks were eliminated using two decoupling frequencies to selectively remove the methylene and hydroxyl protons of the solvent. Comparisons with specifically α-deuterated homo-oligopeptides gave complete assignments of the NH region of the Boc-Met_n-OMe oligomers up to the heptapeptide. Analysis of chemical shifts, coupling constants, and temperature dependence of chemical shifts suggests that up to the hexapeptide, similar structures exist in deuterochloroform and TFE. In contrast, nmr parameters at the heptapeptide for several internal residues differ in these solvents. These results suggest that a C₇ to α-helix transition may occur in TFE as the chain length of the methionine oligopeptides increases.     

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.     

Alkylated poly(amino acids). I. Conformational properties of poly(Nε-trimethyl-L-lysine) and poly(Nδ-trimethyl-L-ornithine)

Poly(N^ε-trimethyl-L -lysine), [Lys(Me₃)]_n, and poly(N^δ-trimethyl-L -ornithine), [Orn(Me₃)]_n, in sodium dodecylsulfate do not assume the β-structure or α-helix, respectively, of their parent polymers. In 0.5M Ca(ClO₄)₂ both [Lys(Me₃)]_n and [Orn(Me₃)]_n are aggregated and display CD spectra indicative of a regular, perhaps helical, structure. For [Lys]_n and [Lys(Me₃)]_n, the T₁ of the α-hydrogens are 0.379 and 0.230 sec, respectively, indicating greater rigidity for [Lys(Me₃)]_n. The CD spectrum of [Lys(Me₃)]_n at pH 8 is more heat resistant than that of [Lys]_n. It is suggested that apolar interactions are more important in the methylated polymers than in the parent polymers.     

A high-resolution 13C-nmr study of collagenlike polypeptides and collagen fibrils in solid state studied by the cross-polarization–magic angle-spinning method. Manifestation of conformation-dependent 13C chemical shifts and application to conformational characterization

We have recorded high-resolution ¹³C-nmr spectra of collagen fibrils in the solid state by the cross-polarization–magic-angle-spinning(CP–MAS)method and analyzed the spectra with reference to those of collagenlike polypeptides. We used two kinds of model polypeptides to obtain reference ¹³C chemical shifts of major amino acid residues of collagen (Gly, Pro, Ala, and Hyp): the 3₁-helical polypeptides [(Gly)_nII, (Pro)_nII, (Hyp)_n, and (Ala? Gly? Gly)_nII], and the triple-helical polypeptides [(Pro? Gly? Pro)_n and (Pro? Ala? Gly)_n]. Examination of the ¹³C chemical shifts of these polypeptides, together with our previous data, showed that the ¹³C chemical shifts of individual amino acid residues are the same, within experimental error (±0.5 ppm), among different polypeptides with different primary sequences, if the conformations are the same. We found that the ¹³C chemical shifts of Ala residues of the 3₁-helical (Ala? Gly? Gly)_n and triple-helical (Pro? Ala? Gly)_n are significantly displaced, compared with those of the α-helix, β-sheet, and silk I form, and can be utilized as excellent probes to examine conformational features of collagen-like polypeptides. Further, the ¹³C chemical shifts of Gly and Pro residues in the triple-helical polypeptides are substantially displaced from those found in (Gly)_nII and (Pro)_nII of the 3₁-helix, reflecting further conformational change from the 3₁-helix to the supercoiled triple helix. In particular, the ¹³C chemical shifts of Gly C ? O carbons of the triple-helical polypeptides are substantially displaced upfield (4.1–5.1 ppm), with respect to those of the 3₁-helical polypeptides. These displacements are interpreted by that Gly C ? O of the former is not involved in NH …? O ? C hydrogen bonds, while this carbon of the latter is linked by these kinds of hydrogen bonds. On the basis of these ¹³C chemical shifts, as reference data for the collagenlike structure, we were able to assign the ¹³C-nmr peaks of Gly, Ala, Pro, and Hyp residues of collagen fibrils, which are in good agreement with the values expected from the model polypeptides mentioned above. We also discuss a plausible conformational change of collagen fibrils during denaturation.     

Vibrational circular dichroism in amino acids and peptides. 7. Amide stretching vibrations in polypeptides

Vibrational circular dichroism (VCD) spectra for the principal amide stretching vibrations, amide A (N? H stretch) and amide I (predominantly C?O stretch), are presented and analyzed for a variety of polypeptides dissolved in chloroform, as well as for two examples in D₂O. Our results for poly(γ-benzyl-L -glutamate) confirm the first and only previous report of VCD in polypeptides carried out by Singh and Keiderling [(1981) Biopolymers 20 , 237–240]. Collectively, our spectra show that the sense of the bisignate VCD in these two regions depends on the sense of α-helicity and not on the absolute configuration of the constituent amino acids. This conclusion is established by obtaining VCD for the two polypeptides, poly(β-benzyl-L -asparate) and poly(im-benzyl-L -histidine), that form left-handed as opposed to right-handed α-helices. A new amide band having significant VCD intensity owing to its Fermi resonance interaction with the N? H stretching mode has been identified as a weak shoulder on the low-frequency side of the amide A band near 3200 cm^?1 and is assigned as a combination band of the amide I and amide II vibrations. VCD spectra of polypeptides in D₂O solution, although weak, have been successfully measured in the amide I region, where spectra appear to be more complicated due to the presence of solvated and internally hydrogen-bonded amide groups. Strong monosignate contributions to the VCD in the amide A and amide I regions for some of the polypeptides indicate coupling of an electronic nature between these two regions and is deduced by an application of the concept of local sum rules of rotational strength. It appears that a detailed understanding of the VCD obtained for polypeptides will not only be diagnostic of secondary structure, but also of more subtle structural and vibrational effects that give rise to local, intrinsic chirality in the amide vibrations.     

Block sequential polypeptides of L-alanine and glycine with D, L-glutamic acid

Sequential polypeptides of L -alanine(A) and glycine(G), which were incorporated between two blocks of poly(D ,L -glutamic acid) (DL), were synthesized by applying Merri-field's solid-phase method. On the basis of optical rotatory dispersion criteria, DL(A)₃₈-DL was found to assume the α-helix in the whole range of the water-methanol system; whereas other block sequential polypeptides were found to assume the random-coiled conformation in water and partly the α-helix at the high methanol content. The stability of the α-helix decreased in the order: DL(A)₃₈DL, DL(A₂G)₁₀DL, DL(A₂G)₆DL, and DL(A₃G)₇DL. This phenomenon may be explained in terms of the dependence of hydrophobic bonding between the C₃H group of the ith L -alanine regularly arranged on the surface of the α-helix and the C₂H group of the (i + 3)th residue on whether the residue is alanine or glycine. The role which the methanol plays in stabilizing the α-helix is also discussed.