The conformation of poly-L-alanine in hexafluoroisopropanol

High-molecular-weight poly-L -alanine dissolved in hexafluoroisopropanol exhibits infrared, ultraviolet, circular dichroism, and optical rotatory dispersion spectra which are unique and unlike any other previously reported polypeptide spectra. Strong evidence that a helical conformation is present is shown by the high degree of hypochromism in the 187mμ absorption peak and by the positions of the amide infrared bands. The CD and ORD spectra are also similar to those of α-helical polypeptides, though important qualitative and qualitative differences are observed. To explain the novel spectra, which are not mixtures of the spectra of previously reported polypeptide conformations, a new α-helix-like conformation is proposed. The postulated conformation (a doubly hydrogen-bonded helix) is a distorted α-helix in which the peptide carbonyl groups point slightly out from the helix axis and are hydrogen bonded simul taneously both to the NH of the fourth peptide residue to the carboxyl terminal side (as in the classical α-helix), as well as to a solvent molecule's hydroxyl hydrogen.     

The optical rotatory properties of poly- -D-glutamic acid

Measurement of the optical rotatory dispersion spectra of poly-γ-D -glutamic acid (obtained from Bacillus anthracis) dawn to 200 nm wavelength reveal difference between the unionized and ionized froms. The profile of the unionized polyacid shows similarities to those obtained for α-helical polypeptides, although with displaced frequencies of the respective maxima and minima. It is suggested that the relative position and magnitudes of the Cotton effect are consistent with a helical structure such as proposed by Rydon (J. Chem. Soc., 1964 , 1328). The optical rotatory dispersion spectrum of the ionized from resembles those obtained from the β-chain from of α-L polypeptides. From model-building studies an extended chain similer to the β-from would seen the most reasonable structure for the ionized poly-γ-acid to adopt, since the charged groups in such a conformation would be at their maximal distances from each other. Such an ordered structure for a polymer is consistent with the hypotheses put forward in the recent literature that charged polypeptides adopt ordered rather than random-coiled conformations.     

Conformation of poly-L-tyrosine in trimethyl phosphate solution

Absorption, circular dichroism (CD), and optical rotatory dispersion (ORD) measurements were carried out on poly-L -tyrosine in trimethyl phosphate solution over the spectral range 185–600 mμ. There is evidence in the CD spectrum for side chain-side chain interactions in poly-L -tyrosine. ORD and CD data in dimethylformamide and pyridine closely parallel those in trimethyl phosphate, indicating a similarity in conformation of the polymer in all three solvents. In the polarized infrared spectrum both position and polarization of amide A, I, and II bands are characteristic of α-helical polypeptides. Bands corresponding to side chain also exhibit dichroism, suggesting that the side chains are not randomly oriented. Viscosity and light-scattering studies are consistent with α-helical structure for the polymer that, remains rigid over a temperature range of 15–50°C and becomes somewhat flexible at higher temperatures. Optical rotatory properties were found to vary gradually and continuously with temperature over the range of ?30 to +100°C. This suggested that all three electronic transitions of tyrosyl side chain are optically active, and that the side chains have some freedom of motion that decreases with decreasing temperature, disappearing only at about ?30°C.     

Solvent effects on the orientation of naphthalene rings in the side chain of poly-gamma-1-naphthylmethyl-L-glutamate

The orientation of naphthalene rings in the side chain of poly-γ-1-naphthylmethyl-L -glutamate (PNLG) in mixed solvents of dichoroethane (DCE) and hexafluoroisopropanol (HFIP) has been studied together with its conformation by infrared, circular dichroism, and fluorescence spectra. The CD pattern of PNLG varies with the solvent composition while it maintains the α-helical conformation. The fluorescence spectra of PNLG in solution show excimer emission of the naphthalene chromophores. The ratio of intensity of the excimer emission to that of the normal fluorescence decreases as the HFIP component in the solvent increases. It is suggested that the naphthalene rings in the side chain of α-helical PNLG are more rigidly orientated in the solvents of higher HFIP ratio.     

Induced optical activity of acridine orange bound to poly-S-carboxymethyl-L-cysteine

The absorption and rotatory properties of acridine orange-poly-S-carboxymethyl-L -cysteine system in water and in 0.2 M NaCl have been measured at different pH and polymer-to-dye mixing ratios. The absorption spectra indicate that the dyes are bound to the polymer in dimeric or highly aggregated forms. At neutral pH where the polymer is randomly coiled, no optical activity is induced on the absorption bands of bound acridine orange. At acid pH where the polymer has the β-conformation, a pair of positive and negative circular dichroic bands occur at each of the absorption bands, centered around 458 and 261 mμ. The signs of those bands are opposite to those found for α-helical poly-L -glutamic acid. A model for the binding of dye to the β-form polymer is presented, in which dimeric dyes are attached to ionized carboxyl groups and slack one another to form linear arrays on both sides of an extended polypeptide chain. The observed circular dichroism spectra can be explained by the Tinoco's exciton mechanism, based on this model. Low molecular weight poly-S-carboxymethyl-L -cysteine induces quite a different circular dichroism on bound acridine orange.     

Raman scattering of some synthetic polypeptides: poly(gamma-benzyl L-glutamate), poly-L-leucine, poly-L-valine, and poly-L-serine

The Raman spectra of poly-γ-benzyl-L -glutamate, poly-L -leucine, poly-L -valine, and poly-L -serine are reported. For the α-helical polymers, the conformationally sensitive amide I, II, and III modes are observed in the Raman as, well as the infrared. For the β form, the Raman effect, supplies the infrared inactive inphase motion which is useful for the determination of a parallel or antiparallel chain alignment. Modes characteristic of the specific polypeptide are also observed which are insensitive to conformation.     

Rotatory dispersion and circular dichroism of low-molecular-weight poly- -benzyl-L-glutamate

Rotatory dispersion and circular dichroism of low-molecular-weight poly-γ-benzyl-L -glutamate, which was prepared from the N-carboxyanhydride by n-hexylamine initiation at [A]/[I] 3, 4, and 8, have been measured in ethylene dichloride and dioxane at different concentrations. The rotatory properties of the polypeptides are all characterized by a trough at 233 mμ of a negative Cotton effect or by a negative circular dichroic band at 223 mμ. With increasing A/I value or concentration, dextrorotation increases and the negative dichroic band becomes deeper. Both the trough magnitude and the negative ellipticity are linearly dependent on the content of β-structure, and the rotatory parameters for the pure β-structure are estimated by extrapolation of the linear relations. Circular dichroism and infrared spectra of the polypeptides have also been measured in trifluoroethanol, and the effect of solvents on the polypeptide conformation is discussed.     

Raman spectra of poly-L-lysines

The Raman spectra of poly-L -lysine hydrochloride and poly-?-carbobenzoxy-L -lysine in the solid state have been obtained and are consistent with the presence of an α-helical structure. The Raman spectrum of poly-L -lysine in aqueous solution suggests the presence of random coil structures.     

Chiroptical properties of phospholipids

The chiroptical properties of phospholipids were investigated by optical rotatory dispersion and circular dichroism. The spectra of phosphatidylcholine varied with the solvent used. The sign of the circular dichroism effects differed in some cases from previously reported. The results show that it is possible to distinguish different types of phospholipids from each other. The results also show that optical rotatory dispersion and circular dichroism might be a very useful tool for the determination of the configuration of various phospholipids.     

The aggregation of basic polypeptide residues bound to heparin

The molecular basis for heparin interactions with proteins has been explored with l-lysine copolymer: heparin complexes, measuring the conformational change and charge neutralization which accompany the complexation, using optical methods. Previous studies had shown that the basic homopolypeptides (poly-l-lysine, poly-l-arginine) assume α-helical conformation upon interaction with numerous glycosaminoglycans (including heparin). Thus, the unique specificity for heparin in the anticoagulation system (which involves two or more lysine residues on the antithrombin molecule) is not paralleled by the findings with the basic homopolymers.Results with mixed polypeptides, poly(lysine: tyrosine, 1:1) and poly(lysine: phenylalanine, 1.4:1), show that these protein models assume different conformational forms upon complexation with heparin, the former shows a poly-l-lysine-like β-structure circular dichroism spectrum and the latter an α-helical structure. The change in circular dichroism spectra increases with the addition of heparin until the ratio of positive to negative charge is about one. Dye-binding studies of the two copolymer systems reveal that the charged groups of reactants are largely blocked in the polypeptide complexes at a calculated charge ratio equal to one. The data indicate that heparin interaction with the cationic polypeptides causes them to assume either the α-helical or β-structure depending upon the nature of the neighboring uncharged amino acid and its proclivity for α-helix or β-structure.     

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.     

Conformations of poly-L-valine in solution

In order to test theoretical predictions that poly-L -valine can exist in an α-helical conformation, water-soluble block copolymers of L -valine and D , L -lysine were prepared. By carrying out the synthesis on a resin support (with the use of N-carboxyanhydrides) contamination of the individual blocks by any unreacted monomer from the previous block was avoided. A single glycine residue was incorporated at the C-terminus of the chain for use in amino acid analyses. Using optical rotatory dispersion and circular dichroism criteria, about 50% of the short valine block of (D , L -lysine HCl)₁₈-(L -valine)₁₅-(D , L -lysine-HCl)1₆-glycine was found to be in the right-handed α-helical conformation in 98% aqueous methanol, in water, the polymer appears to be a dimer, with the valine block being involved in the formation of an intermolecular β-structure.     

Influence of isopropanol-water solvent mixtures on the conformation of poly-L-lysine

The helix–coil transition of poly-L -lysine (PLL) in water–isopropanol solvent mixtures has been investigated at room temperature by circular dichroism measurements. Within the range of 70%–80% isopropanol concentration (by volume), the polymer undergoes a sharp transition, characterized by the formation of a fully charged α-helical structure. On the basis of some experimental evidence the role of the organic component in solution appears more complicated than that of strengthening the intramolecular hydrogen bonds in the polymer. By analogy with the distribution of the components of alcohol–water mixtures in simple ionic systems, it is thought that only an high co-solvent concentration brings about an extensive and possible cooperative depletion of the clusters of firmly-bound water molecules in the domain of the polylelectrolyte, favoring the transition to the α-helical structure. On the other hand, CD spectral patterns show that the addition of NaCl in the alcohol-rich–water mixtures of charged poly-L -lysine gives rise to a transition from the α-helical to a β-structures conversion obeys a first-order rate law at all times, with a rate constant dependent on solvent composition and ionic strength. In these conditions, the rate of the process is close to that found for the thermally induced α–β transition. Higher polymer concentration and/or ionic strength cause a phase separation of β-PLL, suggesting that in this case interchain reactions (where hydrogen bonding should play the major role) predominate. Titration experiments on charged α-helical poly-L -lysine in 85% or 90% isopropanol mixtures confirm the occurrence of a conformational transition, which takes place within a degree of dissociation α of 0.2–0.75. The transition is accompanied by a visible turbidity, which increases as the titration proceeds. Implications of the solvent distribution around the macroion on the observed conformational phenomena are also discussed.     

Conformational studies on poly-L-tryptophan: circular dichroism and x-ray diffraction studies

Circular dichroism (CD) measurements were carried out on various copolymers of L -tryptophan and γ-ethyl L -glutamate in ethylene glycol monomethyl ether as the solvent. On increasing the L -tryptophan content of the copolymers a gradual change in the CD spectra was observed. The typical spectrum of the right-handedα-helix becomes more and more evident as the L -tryptophan content decreases. On the basis of these results we assumed that no conformational transition occurs on proceeding from pure poly (γ-ethyl L -glutamate) to pure poly-L -tryptophan in ethylene glycol monomethyl ether: therefore the conformation of poly-L -tryptophan should be that of a right-handed α-helix. Moreover we observed that the change in the CD spectra of the copolymers is gradual but not linear on increasing the tryptophan content. The deviations from linearity were attributed to interactions among side-chain chromophores whose contributions to the optical activity are not simply additive. An x-ray analysis carried out on oriented films of poly-L -tryptophan casted from solutions of the polymer in dimethylformamide shows conclusively that the solid-state conformation of the polymer is that, of an α-helix.     

Circular dichroism and proton magnetic resonance studies of random chain poly-L-lysine

The 218-nm peak, characteristic of the circular dichroism of randomly coiled poly-α-amino acids can be demonstrated in solutions of penta-L -lysine, α-glycyl-L -lysine, as well as poly-L -lysine. The thermal stability of the particular state that gives rise to this 218-nm band in the CD is similar for all three peptides. These results eliminate the possibility that poly-L -lysine forms a structure with long-range order in acidic aqueous solution since the stability of such a structure would be expected to be greater for a higher molecular weight polymer than for a pentamer. The intrinsic viscosity of poly-L -lysine of molecular weight 180,000 varies only slightly between 25 and 60°C. The proton magnetic resonance spectra of poly-L -lysine and penta-L -lysine are indistinguishable on the basis of the chemical shift of all resonances, their line widths, and the exchange rates of the N? H protons. This demonstrates that poly-L -lysine does not possess a cooperatively formed ordered structure in acidic solutions. A weak band at 238 nm is observed in the circular dichroism of poly-L -lysine and other peptides. It is suggested that the effects of change in temperature, salt concentration, or polymer on both the magnitude and position of the 238-nm band may be explained if it is assumed that it is a shoulder of a lower wavelength peak.     

Conformational and kinetic studies of synthetic polypeptides by NMR

The α-helix–coil transition of poly-L -leucine, poly-L -alanine and poly-L -methionine in chloroform–trifluoroacetic acid system was studied by nuclear magnetic resonance (NMR) and optical rotatory dispersion (ORD). The kinetics of the hydrogen–deuterium exchange in the peptide was also followed in these polymers by means of NMR. Two types of the NMR spectra and the hydrogen–deuterium exchange reaction were found, corresponding to the high and low molecular weight polypeptides. In high molecular weights, the NH and α-CH resonance lines gave single peaks and the hydrogen–deuterium exchange was expressed as a single first order reaction. In low molecular weights, the NH and α-CH lines were separated into two peaks, corresponding to helical and random-coiled states, respectively, and the exchange react ion was expressed as super-position of a very rapid exchange reaction in the random-coiled part and another slow exchange reaction of the first order in the helical part. These results suggest that the helix–coil interconversion of low molecular weight polypeptides has a longer relaxation time (? 4.5 × 10^?3 sec) than that of high molecular weight polypeptides.     

Critical comparison of the experimental optical activity of helical polypeptides and the predictions of the molecular exciton model

The predictions of the presently accepted molecular exciton model for the optical activity of helical polypeptides are in reasonable agreement with experimental spectra in the accessible wavelength range. However, crucial verification requires the detect of a significant negative rotatory hand just below the accessible range. A computer-oriented method is utilized to obtain information concerning the inaccessible range. Optical rotatory dispersion computed by evaluation of the Kronig-Kramers integral transform from the experimentally determined circular dichroism of several helical homopolypeptides in solution are compared with the experimentally determined optical rotatory dispersion. Computed and experimental curves are congruent within an uncertainty approaching that of the experimental technique, whatever the polypeptide sample lot, side chains, and solvent. It is shown that t his agreement is not a computational or experimental artifact. These results can be interpreted in two ways: (1) that the predicted band does not exist, and (2) that the perturbation of the predicted band is being negated by other inaccessible bands in the vacuum ultraviolet. Arguments are presented to show that the first of these two possibilities is more probable.     

Optical Rotatory Dispersion of Polypeptides in the Near-Infrared Region

For the first time ORD measurements in the near-infrared region from 0.7 to 2.0 μ for well-known polypeptides, namely, poly(γ-benzyl L -glutamate), poly(L -glutamic acid), poly-L -lysine·HCl, poly-S-carbobenzoxymethyl-L -cysteine, and Bombyx mori silk fibroin, were carried out. It was found that the value of the optical activity infrared term, which is proportional to the sum of rotational strengths of vibrational transitions, depends on polypeptide conformation. The optical activity infrared term value is equal to zero for the random-coil conformation, it is small but exceeds the measurement error for the α-helical state, and finally, for the β conformation it is an order of magnitude higher than for the α-helical state. The obtained results permit one to hope that on the basis of ORD measurement in the near-infrared region it will be possible to suggest a method of determining the β-form content in polypeptides and proteins     

The circular dichroism spectrum of poly-L-acetoxyproline

We report the circular dichroism (CD) spectrum of poly-L acetoxyproline in trifluoroethanol, a solvent in which the form I to form II conformational isomerization occurs slowly enough to permit observation of the spectral changes. A comparison is made to poly-L proline. As judged by the similarity of the CD spectra, the conformations of the corresponding forms of the two polymers must be nearly the same. Transition assignments are proposed; these are shown to agree with the theoretical calculations of Pysh. There is a serious unexplained discrepancy between our solution data and those of Fasman for poly-L acetoxyproline.     

Raman scattering of chymotrypsinogen A, ribonuclease, and ovalbumin in the aqueous solution and solid state

The Raman spectra of three globular proteins, beef pancreas chymotrypsinogen A, beef pancreas ribonuclease, and hen egg white ovalbumin have been obtained in the solid state and aqueous solution. X-ray diffraction and circular dichroism evidence have indicated that these proteins have a low α-helical content and a large fraction of the residues in the unordered and β-sheet conformation. The frequencies and intensities of the amide I and amide III lines are consistent with assignments based on the Raman spectra of polypeptides. The intense amide III lines observed in all the spectra would be expected for proteins with a low fraction of the residues in the α-helical conformation. Several spectra changes occur upon dissolution of the proteins in water and may be associated with further hydration of the proteins. The spectrum of thermally denatured chymotrypsinogen is presented. A 3 cm^–1 decrease in the frequency of the amide I line of the protein dissolved in D₂O upon heating was observed. This observation is consistent with a denaturation mechanism allowing only slight changes in the secondary structure but an increase in solvent penetration upon going from the native to the reversibly denatured state.