Conformational Analysis of the β-amyloid Peptide Fragment, β(12–28)

Abstract

NMR and CD spectroscopy have been used to examine the conformation of the peptide, β(12–28), (VHHQKLVFFAEDVGSNK) in aqueous and 60% TFE/40% H₂0 solution at pH 2.4. In 60% TFE solution, the peptide is helical as confirmed by the CD spectrum and by the pattern of the NOE cross peaks detected in the NOESY spectrum of the peptide. In aqueous solution, the peptide adopts a more extended and flexible conformation. Broadening of resonances at low temperature, temperature-dependent changes in the chemical shifts of several of the CH_α resonances and the observation of a number of NOE contacts between the hydrophobic side-chain protons of the peptide are indicative of aggregation in aqueous solution. The behavior of β(12–28) in 60% TFE and in aqueous solution are consistent with the overall conformation and aggregation behavior reported for the larger peptide fragment, β(1–28) and the parent β-amyloid peptide.     

Conformational studies of poly-L-alanine in water

The conformational properties of poly-L -alanine have been examined in aqueous solutions in order to investigate the influence of hydrophobic interactions on the helix–random coil transition. Since water is a poor solvent for poly-L -alanine, water-soluble copolymers of the type (D , L -lysine)_m–(L alanine)_n-(D , L -lysine)_m, having 10, 160, 450, and 1000 alanyl residues, respectively, in the central block, were synthezised. The optical rotatory dispersion of the samples was investigated in the range 190–500 mμ, and the rotation at 231 mμ was related to the α-helix content, θ_H, of the alanine section. In salt-free solutions, at neutral pH, the three large polymers show high θ_H values, which are greatly reduced when the temperature is increased from 5 to 80°C. No helicity was observed for the small (n = 10) polymer. By applying the Lifson-Roig theory, the following parameters were obtained for the transition of a residue from a coil to a helical state: ν = 0.012; ΔH = ?190 ± 40 cal./mole; ΔS = ?0.55 ± 0.12 e.u. Since ΔH and ΔS differ from the values expected for a process involving only the formation of a hydrogen bond, and in a manner predicted by theories for the influence of hydrophobic bonding on helix stability, it is concluded that a hydrophobic interaction is also involved. In the presence of salt (0.2M NaCl), or when the ε-amino groups of the lysyl residues are not protonated (pH = 12), the helical form of the two large polymers (n = 450 and n = 1000) is more stable than in water. Since the electrostatic repulsion between the lysine end blocks is greatly reduced under these conditions, the alanine helical sections fold back on themselves, and this conformation is stabilized by interchain hydrophobia bonds. This structure was predicted by the theory for the equilibrium between such interacting helices, non-interacting helices, and the random coil.     

Raman spectra of D and L amino acid copolymers. Poly-DL-alanine, poly-DL-leucine, and poly-DL-lysine.

The Raman spectrum of poly-DL -alanine (PDLA) in the solid state is interpreted in terms of the disordered chain conformation, in analogy with the spectrum of mechanically deformed poly-L -alanine. The polymer is largely disordered with only a small α-helical content in the solid state. When PDLA is dissolved in water, the spectra suggest that short α-helical segments are formed upon dissolution. These helical regions might be stabilized by hydrophobic bonds between side-chain methyl groups. Addition of methanol to the aqueous PDLA solutions results in a Raman spectrum resembling that of solid PDLA. This result suggests that the methanol disrupts the helical regions by breaking the hydrophobic bonds. The Raman spectra of poly-DL -leucine (PDLL) and poly-L -leucine (PLL) are compared and only slight differences are observed in the amide I and III regions, indicating that PDLL does not have an appreciable disordered chain content. Significant differences are observed in the skeletal regions. The 931-cm^?1 lines in the PLL and PDLL spectra are assigned to residues in α-helical segments of the preferred screw sense, i.e., L -residues in right-handed segments and D -residues in left-handed segments (in PDLL). On the other hand, the 890-cm^?1 line in the spectrum of PDLL is assigned to residues not in the preferred helical sence, i.e., L -residues in left-handed segments and D -residues in right-handed ones. The Raman spectra of poly-DL -lysine and poly-L -lysine in salt-free water at pH 7.0 are compared. The Raman spectra of the two polymers are very similar. However, this does not negate the hypothesis of local order in poly-L -lysine because the distribution of the residues in poly-DL -lysine probably tends towards blocks, and the individual blocks may take up the 3₁ helix.     

Steric structure of L-proline oligopeptides. II. Far-ultraviolet absorption spectra and optical rotations of L-proline oligopeptides

The results of the measurement of the far-ultraviolet absorption spectra of L -proline oligomers in water and acetonitrile are summarized as follows. The monomer has an absorption maximum at 182.5 mμ in acetonitrile. The absorption maximum of the dimer is found at 185 mμ and a shoulder appears around 200 mμ, that is, splitting of the absorption spectrum is observed in the dimer. As the degree of polymerization increases, the position of the shoulder shifts toward the wavelength of the absorption maximum of poly-L -proline II, with an accompanying increase in intensity. We may describe the absorption peak around 203 mμ of poly-L -proline II as identical with the shoulder with an increased intensity. By measurements of optical rotatory dispersion and circular dichroic spectra, it was also confirmed that the appearance of the helical conformation commences at the tetramer. When the number of residues is five or greater, the conformation of the helical structure of poly-L -proline II seems to be completed.     

Conformational studies of proteins with aromatic side-chain effects

We present here a brief analysis of ultraviolet isotropic absorption and related circular dichroism of the n–π* and π–π* transitions for the peptide (amide) chromophore in the 185–240 mμ region. Investigations by ultraviolet absorption and circular dichroism techniques on natural amino acids with aromatic chromophores in their side chains are also reported. By taking into account both the peptide and aromatic transitions we discuss the conformational studies of proteins with aromatic side-chain effects. Our attention is largely focused on the optical rotatory dispersion and circular dichroism spectra of these proteins in the near ultraviolet region, where characteristic aromatic side-chain bands occur. The 185–240 mμ region is also discussed when evidence exists of overlapping Cotton effects of aromatic and peptide groups.     

Synthesis and conformational study of poly(N delta-carbobenzoxy, N delta-benzyl-L-ornithine) and poly(N delta-benzyl-L-ornithine)

Poly(N^δ-carbobenzoxy, N^δ-benzyl-L -ornithine) (PCBLO) was prepared by the standard NCA method. PCBLO was converted into poly(N^δ-benzyl-L -ornithine) (PBLO) through decarbobenzoxylation with hydrogen bromide. The monomer N^δ-benzyl-L -ornithine was synthesized by reacting L -ornithine with benzaldehyde, followed by hydrogenation. The conformation of the two polypeptides was studied by optical rotatory dispersion and circular dichroism. PCBLO forms a right-handed helix in helix-promoting solvents. In mixed solvents of chloroform and dichloroacetic acid (DCA) it undergoes a sharp helix–coil transition at 12% (v/v) DCA at 25°C, as compared with 36% for poly(N^δ-carbobenzoxy-L -ornithine) (PCLO). Like PCLO, the helix–coil transition is “inverse,” that is, high temperature favors the helical form. PBLO is soluble in water at pH below 7 and has a “coiled” conformation. In 88% (v/v) 1-propanol above pH (apparent) 9.6 it is completely helical. In 50% 1-propanol the transition pH (apparent) is about 7.4; this compares with a pH_tr of about 10 for poly-L -ornithine in the same solvent.     

Raman spectroscopic study of mechanically deformed poly-L-alanine

Raman spectroscopy has been used in investigating the conformational transitions of poly-L -alanine (PLA) induced by mechanical deformation. We see evidence of the alpha-helical, antiparallel beta-sheet, and a disordered conformation in PLA. The disordered conformation has not been discussed in previous infrared and X-ray diffraction investigations and may have local order similar to the left-handed 3₁ poly glycine helix. The amide III mode in the Raman spectrum of PLA is more sensitive than the amide I and II modes to changes in secondary structure of the polypeptide chain. Several lines below 1200 cm^?1 are conformationally sensitive and may generally be useful in the analysis of Raman spectra of proteins. A line at 909 cm^?1 decreases in intensity after deformation of PLA. In general only weak scattering is observed around 900 cm^?1 in the Raman spectra of antiparallel beta-sheet polypeptides. The Raman spectra of the amide N–H deuterated PLA and poly-L -leucine (PLL) in the alpha-helical conformation and poly-L -valine (PLV) in the beta-sheet conformation are presented. Splitting is observed in the amide III mode of PLV and the components of this mode are assigned. The Raman spectrum of an alpha-helical random copolymer of L -leucine and L -glutamic acid is shown to be consistent with the spectra of other alphahelical polypeptides.     

Effect of side-chain hydrophobic bonding on the stability of homopolyamino acid alpha-helices: conformational studies of poly-l-leucine in water

The conformational properties of block copolymers of poly-L -leucine in water have been examined. The degree of polymerization of the poly-L -leucine block was 11 and 21, respectively, for samples prepared by the Merrifield procedure, and 56 for a sample prepared by the polymerization of leucine N-carboxyanhydride. The optical rotatory dispersion parameter b₀ was used to obtain the helix content θ_h at various temperatures. Application of the Lifson-Roig theory gave the following parameters for the transition of a residue from a coil to a helical state: v = 0.05–0.011, ΔH = +100 cal/mole, ΔS = +0.70–1.00 e. u. These parameters, as well as those for other polyamino acids, are accounted for by hydrophobic bonds involving the nonpolar side chains in the helical and randomly coiled forms. From the data for poly-L -alanine and theoretical values of the thermodynamic parameters for hydrophobic bond formation, the parameters for formation of a polyglycine helix are computed. By separating the contributions of the backbone, it is possible to obtain a set of thermodynamic parameters for the side-chain contributions of a number of polyamino acids. Increased size of the nonpolar side chain (with a larger contribution from hydrophobic bonding) makes a larger contribution to the stability of the α-helix which is reflected, among other ways, in a higher helix content at given temperature.     

Far-infrared spectra of polyalanines with alpha-helical and beta-form structures

Far-infrared spectra of poly-L -alanines having the α-helical conformation and the β-form structure were measured. The spectra of glycine–L -alanine copolymer, silk fibroin, and copoly-D ,L -alanines with different D :L compositions were also measured. In addition to the bands so far reported, four bands at 190, 107, 120, and 90 cm^?1were found for the α-helix conformation and the two bands at 442 and 247 cm^?1 were found for the β form. The 442 cm^?1 band consists of the parallel 432 cm^?1 and perpendicular 445 cm^?1 bands. The 247 cm^?1 band is well defined and has strong dichroism parallel to the direction of stretching. These two bands appear also for silk fibroin and glycine–L -alanine copolymer. All the far-infrared bands of copoly-D ,L -alanines can be interpreted as α-helix bands, the three peaks at 580, 478, and 420 cm^?1 being ascribed to the D -residue incorporated into the right-handed α-helix or to the L -residue in the left-handed α-helix.     

Far-infrared spectra of poly(-α-amino acids) with basic alkyl group side chains

Far-infrared spectra in the region from 700 to 60 cm^?1 have been measured for the α-helix structures of poly(L -α-amino-n-butyric acid), poly-L -norvaline, poly-L -norleucine, and poly-L -leucine and for the β-form structures of poly(L -α-amino-n-butyric acid), poly-L -valine, poly(DL -amino-n-butyric acid), poly-DL -norvaline, and poly-DL -norleucine. The changes of the spectra on N-deuteration have been measured in the region between 700 and 400 cm^?1. It is concluded that, the α-helix has characteristic bauds near 690, 650, 610, 380, 150, and 100 cm^?1, and that the β-form has characteristic bands near 700, 240, and 120 cm^?1. The main-chain vibrations in the region from 600 to 200 cm^?1 are strongly coupled with the side-chain deformation vibrations.     

Optical rotatory dispersion and circular dichroism of carbanilyl polysaccharides

Measurements of optical rotatory dispersion (ORD) and circular dichroism (CD) have been made in the range of 600-210 mμ for the β-glycan carbanilates as for instance, 2,3,6-tricarbanilylcellulose (I), 2,3,6-tricarbanilylmannan (II), 2,3-dicarbanilylcellulose (III), and octacarbanilylcellobiose (IV) and also for the α-glycan carbanilates, such as 2,3,6-tricarbanilylamylose (V), tricarbanilylpullulan (VI), 2,3-dicarbanilylamylose (VII), and octacarbanilylmaltose (VIII). Furthermore, the 2,3,4,6-tetracarbanilyl-α-methyl-glucopyranoside (IX) and the 1,2,3,4,6-pentacarbanilylglucose (X) have been measured in dioxane at 20°C. For the β-glycans a small negative CD in the region of 238–240 mμ and nearly symmetrical ORD curve with a crossover point at 238–240 mμ are found; this indicates a simple negative Cotton effect. In the case of α-glycosides, a strong negative CD with a maximum at 240–242 mμ and a strong positive CD with a maximum at 223–225 mμ were found; the ORD curves are asymmetrical and cross the abscissa in two places, at 241–243 and 220–222 mμ. With 2,3,4,6-tetracarbanilyl-α-methylglucoside (IX) no CD and ORD in the ultraviolet region and with 1,2,3,4,6-pentacarbanilyl-glucopyranoside (X) the ORD, but not the CD, could be measured. The ORD curve is nearly symmetrical, like those of the β-glycans but is of opposite sign. It seems impossible to discuss the striking difference of the CD and ORD spectra between the α-and the β-glycans in terms of contributions of single independant chromophores influenced by their individual different steric arrangements and their spatial relation to the glycosidic bond in C₁. The exciton theory of Moffitt, which is suitable for explaining the ORD and CD spectra of helical polymers, has been applied to α- and β-glycans. A structure with helical parts is proposed for the α-glycans while a nearly planar arrangement is assumed for the β-glycans.     

Conformations of copoly(gamma-benzyl L-glutamate-O-benzyl-L-serine)

Four samples of copolymers of γ-benzyl is L -glutamic (BLG) and O-benxyl-L -serine (BLS) were synthesized by changing the mixing ratio of two monomer anhydrides. The conformations of these copolymers in CHCl₃, containing very small amount of dichloroacetic acid (DCA) necessary to dissolve the sample, were determined by their compositions; the copolymer which is rich in BLG is mostly helical and one which is rich in BLS is mostly in the β conformation. However, in DCA solution the conformations of these copolymers are independent of their composition. The interesting observation was that the copolymer which has least con tent of BLS is richest in β-conformation.     

Solution conformation study of substance P methyl ester and [Nle10]-neurokinin A (4–10) by nmr spectroscopy

High-resolution proton spectra at 500 MHz of two tachykinin peptides, substance P methyl ester (SPOMe) and [Nle¹⁰]-neurokinin A (4–10), have been obtained in dimethylsulfoxide (DMSO), and for SPOMe, also in 2, 2, 2-trifluoroethanol (TFE)/water mixtures. Complete chemical shift assignments for these peptides were made based on two-dimensional (2D) nmr techniques, correlated spectroscopy and total COSY. J coupling measurement and nuclear Overhauser effect spectroscopy (NOESY) were then used to determine the conformation of these peptides in the various solvents. Based on the J coupling, NOE correlations, and temperature coefficients of the NH resonances, it is concluded that these two peptides exist in DMSO at room temperature as a mixture of conformers that are primarily extended. For SPOMe in TFE/water with high TFE content, however, helical structures are found to be present, and they become quite clear at temperatures between 270 and 280 K. The variation of the ¹³C chemical shifts of the C_α (the secondary shift) with TFE contents corroborates this conclusion. The NOE and C_α shifts show that the main helical region for SPOMe lies between ⁴P and ⁹G. The C-terminus segment L? M? NH₂ is found to be quite flexible, which appears to be quite common for neurokinin-1 selective peptides. © 1993 John Wiley & Sons, Inc.     

Synthesis and conformational study of poly(N -benzyl-L-lysine) and its benzyloxycarbonyl derivative

The solvent-and pH-induced conformational changes are examined in order to investigate the influence of benzyl group. Polymer was prepared via N^?-benzyloxycarbonyl, N^?-benzyl-N^α-carboxy-L -lysine anhydride. The resulting poly (N^?-benzyloxycarbonyl, N^?-benzyl-L -lysine) was obtained in high yield and had a high molecular weight. The protected polymer was removed into poly (N^?-benzyl-L -lysine) by treating it with hydrogen bromide. From the results of the ORD and CD, the protected polymer has a righthanded α-helix, showing [m′]₂₃₃ = –10,300, [θ]₂₂₀ = –27,600 and [θ]₂₀₇ = –25,100 in dioxane. The breakdown of the helical conformation is found to occur at 8% dichloroacetic acid in chloroform-dichloroacetic acid mixture. In the pH range 3.35–6.90, poly (N^?-benzyl-L -lysine) is in a random coil structure. In the pH range 7.50–13.0, the polypeptide has a right-handed α-helix structure; [m′]₂₃₃ = –12,000, [0]₂₂₀ = –27,200, and [0]₂₀₇ = –27,000. In comparison with poly-L -lysine, the coil-to-helix transition is observed at lower pH range in 50% n-propanol. Above pH 8 by heating, the α ? β transition of poly (N^?-benzyl-L -lysine) is not observed in an aqueous media.     

Circular dichroic spectrum of poly-L-tyrosine in aqueous solution

The UV and CD spectra of poly-L-tyrosine were investigated at pH 10.6 and pH 11.2. At pH 10.6 (μ=0.1), the CD spectrum exhibits a medium positive band at 230mμ, an extremely small negative band at 217mμ, and a large positive band at 200mμ. At pH 11.2 (μ=0.1), a new positive CD band appears at 277mμ while the bands at 230mμ and 217mμ are shifted to longer wavelengths by 15 and 10mμ respectively. These results, together with UV spectral data and a specific rotation- pH profile, suggest that at pH 10.6, poly-L-tyrosine exists in the helical conformation with only a small fraction of its side chains ionized; at pH 11.2, the polypeptide retains its helical structure but with a considerable increase in ionization.     

NMR studies in solution of poly-L-proline

The isomerization of poly-L -proline in different solvents has been studied by NMR spectroscopy. Different resonance signals for the CH_α protons have been obtained for the two different helical conformations of thus compound, namely form I and form II.     

Helix–random chain transitions of polyamino acids in organic acid–salt solutions

Polyamino acids which are soluble and helical in acetic acid and dichloroacetic acid (DCA) have been observed to undergo a helix to random chain transition upon the addition of lithium salts of strong acids. The transition can be reversed by diluting the salt. Apparently only lithium cations are able to bring about the polycarbobenzoxy-L -lysine (PCBL) transition in acetic acid, whereas the anions display a varying degree of effectiveness; ClO₄^? > Br^? > TSA^? > Cl^? > NO₃^?. The lithium salts of carboxylate anions such as OAc^? and TFA^? do not cause polymer unwinding in acetic acid. Neither do the acids, TSA, HCl, TFA, or DCA induce the transformation in acetic acid. Poly-L -alanine (PLA) in DCA unfolds as LiBr is added, but does not unfold in the presence of 0.5M (CH₃)₄NBr, 0.25M CsBr, or 0.32M HCl. These results are explained on the basis of a direct interaction of the lithium salt with the polymer amide groups to form an ion-pair complex. The extent to which the union of the ion pair can dissociate from the complex in the low dielectric constant, environment determines the degree of unfolding of the polymer. The anion dissociation equilibrium presumably therefore would lie in the same order as given above. Acids such as HCl and TSA are considered to substantially protonate and ion-pair with the polymer, but do not readily dissociate the anion partner from the complex, and therefore do not produce an unstable positively charged helical structure.     

Helix formation in model peptides based on nucleolin TPAKK motifs

The structures formed by peptide models of the N-terminal domain of the nucleolar protein nucleolin were studied by CD and nmr. The sequences of the peptides are based on the putative nucleic acid binding sequence motif TPAKK: The peptides TP1 and TP2 have the sequence acetyl-G(ATPAKKAA)_nG-amide, with n = 1 and 2, respectively. CD measurements indicate structural changes in both peptides when the lysine side chains are uncharged by increasing the pH or acetylation of the side-chain amines. When trifluoroethanol (TFE) is added, more extensive structural changes are observed, resembling helical structure based on nmr nuclear Overhauser effect (NOE) and C^α proton chemical shift changes, and CD spectra. The structure formed in 0.5M NaClO₄ as observed by nmr is similar to that when the lysine side chains are acetylated, due presumably to interactions of perchlorate ion with side-chain charges on lysines. The helical structure observed in TPAKK motifs may be stabilized via N-capping interactions involving threonine. The structures observed in TFE suggest that the Thr-Pro sequence initiates short helical segments in TPAKK motifs, and these helical structures might interact with nucleic acids, presumably via interactions between lysines and threonines of nucleolin. © 1995 John Wiley & Sons, Inc.     

Conformational studies on polypeptides. The effect of sodium perchlorate on the conformation of poly-L-lysine and of random copolymers of L-lysine and L-phenylalanine in aqueous solution

Circular Dichroism measurements have been carried out on poly-L -lysine (PLL) and on random copolymers of lysine and phenylalanine at various p^H values and in the presence of different amounts of NaClO₄. The results indicate that either the homopolymer or the copolymers at p^H conditions at which the side-chain amino groups are fully protonated, assume the right-handed α-helical conformation in the presence of NaClO₄. The results are interpreted in terms of specific binding of ClO₄^? ions on charged side-chain amino groups.     

Conformational studies on a modified poly-L-tryptophan: Circular dichroism and optical rotatory dispersion of poly-2-(2-nitrophenylsulfenyl)-L-tryptophan and of random copolymers of L-tryptophan and 2-(2-nitrophenylsulfenyl)-L-tryptophan

Optical rotatory dispersion (ORD) and circular dichroism (CD) measurements were carried out on a block copolymer, (γ-ethyl DL -glutamate)₁₆₀ (L -Trp)₃₂, in which the tryptophan sequence has been modified to various extents by using 2-nitrophenylsulfenyl chloride. The CD spectrum of the completely modified copolymer exhibits bands in some of the regions of maximum absorption of the sidechain chromophores. In the peptide absorption region the spectrum is similar to that reported in the literature for polypeptides in the α-helical conformation. When the extent of modification of the tryptophan sequence is progressively reduced, there is a gradual change in the ORD spectra of the copolymers. On the basis of these data the assumption was made that no conformational change occurs on proceeding from the pure unmodified tryptophan sequence to the completely modified sequence. The results are discussed in connection with the study of possible conformational effects arising from selective chemical modification of tryptophan residues in proteins.