Small-angle x-ray scattering by poly-L-alanine solutions

The radius of gyration and “persistence length” of poly-L -alanine, calculated from small-angle x-ray scattering data, have values of 56 Å and 44 Å, respectively, in dichloroacetic acid, and 78 Å and ～30 Å in a 1:1 v/v mixture of trifluoroacetic acid and trifluoroethanol. This can be interpreted to mean that poly-L -alanine exists in a relatively rigid, predominantly α-helical conformation in dichloroacetic acid and in an extended, more flexible form in the mixed solvent system.     

Proof of the charging of polypeptides and polyamides in organic acids

The electrophoresis of poly-γ-benzyl-L -glutamate (PBLG), poly-L -alanine (PLA) and nylon dissolved in various solvents was studied in a glass cell containing three sintered glass partitions. After the passage of a measured amount of charge the concentration of PBLG remained constant in all four chambers when the helicogenic solvents dimethylformamide and ethylene dichloride were used, but in mixtures of ethylene dichloride and dichloroacetic acid and in trifluoroacetic acid, polypeptide migrated to the cathode. Electrophoresis also occurred with PLA in trifluoroacetic acid and with nylon in formic acid. Although the total charge on the polyion could not be determined, the results show beyond reasonable doubt that polypeptides and polyamides are protonated in the presence of moderately strong organic acids.     

Nuclear magnetic resonance investigation of the helix in random coil transformation in poly-alpha-amino acids. I

High-resolution nuclear magnetic resonance spectra at 100 MHz and 220 MHz have been obtained on two samples of poly-L -alanine of differing molecular weights (2500 and 42 500) in the chloroform–trifluoroacetic acid system under various conditions of solvent composition, temperature, and polypeptide concentration. Separate helix and random coil peaks are observed for the α-CH and peptide NH backbone proton resonances, thereby permitting the determination of helix content. This observation of separate peaks demonstrates that the lifetimes of the helix and random coil portions of poly-L -alanine have lower limits of about 10^?1 sec. It is suggested that solvent–peptide versus peptide–peptide hydrogen bond competition, coupled with a destabilizing effect of the trifluoroacetic acid on the helix, is responsible for the helix–random coil transformation.     

Synthesis and conformational study of poly(0,0′-dicarbobenzoxy-L-β-3,4-dihydroxyphenyl-α-alanine)

High-molecular-weight poly(0,0′-dicarbobenzoxy-L -β-3,4-dihydroxyphenyl-α-alanine) was prepared by the N-carboxyanhydride method. From the results obtained by a study of the optical rotation, nuclear magnetic resonance, and solution infrared absorption, the conformation of poly(0,0′-dicarbobenzoxy-L -β-3,4-dihydroxyphenyl-α-alanine) depended greatly on the solvent taking a right-handed helix with [θ]₂₂₅ = ?13,600 ～ ?18,900 in alkyl halides, a left-handed helix with [θ]₂₂₈ = 22,100 ～ 24,800 in cyclic ethers or trimethylphosphate, and a random coil structure in dichloroacetic acid, trifluoroacetic acid, or hexafluoroacetone sesquihydrate. The polypeptide underwent a right-handed helix-coil transition in chloroform/dichloroacetic acid (or trifluoroacetic acid) mixed solvents and a left-handed helix-coil transition in dioxane/dichloroacetic acid (or trifluoroacetic acid) mixed solvents. The results were compared with those of poly(0-carbobenzoxy-L -tyrosine).     

Vibrational spectrum of cyclic tetra-L-alanine

A normal coordinate analysis for cyclic tetra-L -alanine molecule is reported. A comparison of amide modes and other low-frequency vibrations sensitive to conformational changes is made with those in poly-L -alanine. Intramolecular coupling coefficients are calculated using perturbation treatment.     

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.     

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.     

Low-frequency vibrational spectra of some homopolypeptides in the solid state

Low-frequency Raman and far-infrared spectra of polyglycine, poly-L -alanine, and poly-L -valine have been measured. The Raman spectra exhibit an intense band near 100 cm^?1 for these homopolypeptides. Lattice calculations of the polyglycines are used to assign the intense Raman band to a rotary lattice mode. For homopolypeptides in the β conformation, an infrared band is observed whose frequency varies inversely with the square root of the mass of the peptide repeating unit. This infrared band is assigned to the hydrogen bond stretching lattice vibration.     

Vibrational frequencies and modes of alpha-helix

Dichroic properties of the far-infrared absorption bands of the right-handed α-helix of poly-L -alanine were measured. The normal vibration frequencies of this structure were calculated. The assignments of bands were made and the vibrational modes dis-cussed. The frequencies of the α-helix vibrations with various phase differences were calculated. The frequencies of accordionlike vibrations and Young's modulus of the α-helix were estimated. The vibrational frequency for the right-handed α-helices of poly-D -alanine and poly(L -α-amino-n-butyric acid) were calculated, and the results were used for the interpretation of the spectra of copoly-D ,L -alanines and poly(L -α-amino-n-butyric acid). For the latter compound the existence of the rotational isomers in the side chain was strongly suggested. The vibrational modes of the bands characteristic of the α-helix were discussed with regard to the results of the normal coordinate treatment.     

Phonon dispersion curves and normal coordinate analysis of -poly-L-alanine

The vibrational frequencies of α-helical poly-L -alanine and its N-deuterated analog have been assigned by normal coordinate analyses. The phonon dispersion curves and frequency distribution of α-poly-L -alanine have been calculated by using a model which includes hydrogen bonding. The frequency distribution was used to interpret the inelastic neutron scattering data and to calculate the heat capacity. The low-frequency chain modes involving accordian-like motions of the whole helix have been calculated and their dispersion investigated by means of a simplified model.     

Raman spectrum of the right-handed α-helix of poly-L-alanine

The laser-excited Raman vibrational spectrum of poly-L -alanine has been obtained. The Raman spectrum is compared with the infrared spectrum and vibrational frequencies calculated from normal coordinate analysis. The symmetric modes of the α-helix appear with strong intensity in the Raman spectrum. A large number of skeletal modes are obtained in this Raman spectrum for the first time.     

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.     

Helix–coil stability constants for amino acids in nonaqueous solvents. Studies of random poly(γ-benzyl-L-glutamate-co-L-alanine) and poly(γ-benzyl-L-glutamate-co-L-leucine) in a mixed solvent

The host–guest technique has been applied to the determination of the helix–coil stability constants of two naturally occurring amino acids, L -alanine and L -leucine, in a nonaqueous solvent system. Random copolymers containing L -alanine and L -leucine, respectively, as guest residues and γ-benzyl-L -glutamate as the host residue were synthesized. The polymers were fractionated and characterized for their amino acid content, molecular weight, and helix–coil transition behavior in a dichloroacetic acid (DCA)–1,2-dichloroethane (DCE) mixture. Two types of helix–coil transitions were carried out on the copolymers: solvent-induced transitions in DCA–DCE mixtures at 25°C and thermally induced transitions in a 82:18 (wt %) DCA–DCE mixture. The thermally induced transitions were analyzed by statistical mechanical methods to determine the Zimm-Bragg parameters, σ and s, of the guest residues. The experimental data indicate that, in the nonaqueous solvent, the L -alanine residue stabilizes the α-helical conformation more than the L -leucine residue does. This is in contrast to their behavior in aqueous solution, where the reverse is true. The implications of this finding for the analysis of helical structures in globular proteins are discussed.     

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.     

Raman spectroscopic study of tropomyosin denaturation

Raman spectra of the pH denaturation of tropomyosin are presented. In the native state tropomyosin has an alpha-helical content of nearly 90%, but this value drops rapidly as the pH is raised above 9.5. The Raman spectrum of the native state is characterized by a strong amide I line appearing at 1655 cm^?1, very weak scattering in the amide III region around 1250 cm^?1, and a medium-intensity line at 940 cm^?1. When the protein is pH-denatured, a strong amide III line appears at 1254 cm^?1 and the 940 cm^?1 line becomes weak. The intensities of the latter two lines are a sensitive measure of the alpha-helical and disordered chain content. These results are consistent with the helix-to-coil studies of the polypeptides. The Raman spectra of α-casein and prothrombin, proteins thought to have little or no ordered secondary structure, are investigated. The amide III regions of both spectra display strong lines at 1254 cm^?1 and only weak scattering is observed at 940 cm^?1, features characteristic of the denatured tropomyosin spectrum. The amide I mode of α-casein appears at 1668 cm^?1, in agreement with the previously reported spectra of disordered polypeptides, poly-L -glutamic acid and poly-L -lysine at pH 7.0 and mechanically deformed poly-L -alanine.     

Neutron-scattering spectroscopy of the alpha- and beta- forms of poly-L-alanine. Motion of the methyl side chain.

Detailed inelastic, incoherent neutron-scattering (INS) spectra are presented for poly-L -alanine in both the α-helical and β-sheet form. Assignments are made from previous normal coordinate calculations. Of particular interest is the methyl torsion at 230 cm^?1, which is the strongest peak in the spectrum and is independent of backbone conformation. The height of the potential barrier for methyl group rotation is calculated to be 14 kJ mol^?1.     

Far ultraviolet optical rotatory properties of poly-L-tryptophan. I

A block copolymer [γ-Et-DL -Glu]_m [L -Trp]_n was prepared using N-carboxy anhydrides (NCA) of L -tryptohan and γ-ethyl DL -glutamate. The block copolymer, dissolved in trifluoroethanol (TFE)–dichloroacetic acid (DCA) mixtures, exhibited a sharp change in the specific rotation at 546 mμ when the solvent composition reached 70–75% DCA content. Optical rotatory dispersion (ORD) and circular dichroism (CD) measurement were carried out in TFE solution in the spectral range 180–350 mμ. Indole side-chain chromophores were found to be optically active in the polymer. On the other hand, these groups exhibit very small optical activity in the model compound C₆H₃? CH₂? O? CO? (L -Trp)₂? O? CH₃. Indole groups therefore appear to be in a dissymmetric environment only in the polymer. From these data it was concluded that poly-L -Trp is in some type of helical conformation in TFE. Strong overlapping of CD bands from side-chain chromophores and peptides chromophores in the wavelength range 185–240 mμ does not allow definite conclusions to be drawn about the type of helical conformation which exists in poly-L -Trp in TFE solution.     

Far-infrared spectra of sequential copolymers of amino acids with alkyl group side chains

Far-infrared spectra were measured for the sequential copolymers of amino acids with alkyl group side chains. The analysis of the spectra showed that (L -Ala-L -Ala-Gly)_n, (L -Ala-Gly)_n, (L -Ala-Gly-Gly)_n, (L -Val-L -Ala-L -Ala)_n, and (L -Val-L -Ala)_n, have the antiparallel pleated sheet structures and that the backbone conformations of (L -Val-L -Val-L -Ala)_n and (L -Val-L -Val-Gly)_n are the same as that of poly-L -valine. The far-infrared bands characteristic of the antiparallel pleated sheet structure were assigned on the basis of the result of the normal coordinate analysis of poly-L -alanine with this structure. The intersheet and interchain spacings of the sequential copolymers with the antiparallel pleated sheet structure were determined from the x-ray powder-diffraction patterns of these samples.     

Conformational studies of poly(L-tyrosine). A helix–coil transition in dimethyl sulfoxide–dichloroacetic acid mixtures

Poly(L -tyrosine) is a random coil in dimethyl sulfoxide. Upon addition of dichloroacetic acid, poly(L -tyrosine) undergoes a conformational transition centered at about 10% dichloroacetic acid. The transition is nearly complete at 20% dichloroacetic acid. Further addition of dichloroacetic acid leads to precipitation of poly(L -tyrosine). We have characterized this transition by optical rotation, viscosity, circular dichroism, and infrared. The optical rotation at 350 nm and the intrinsic viscosity increase sharply to values that are consistent with a transition to the α-helix conformation. The circular dichroism of poly(L -tyrosine) in dimethyl sulfoxide and in dimethyl sulfoxide/dichloroacetic acid (80:20 v/v) agrees with previous reports for random-coil and α-helix conformations, respectively. The infrared spectrum of poly(L -tyrosine) in dimethyl sulfoxide/dichloroacetic acid (80:20 v/v) shows no evidence of β-structure. We conclude that the transition on going from dimethyl sulfoxide to 20% dichloroacetic acid in dimethyl sulfoxide is a coil → α-helix transition. The amide-I band of poly(L -tyrosine) in dimethyl sulfoxide/dichloroacetic acid (80:20) is found to be at 1662 cm^?1. It has been suggested that this high frequency may be indicative of a left-handed α-helix. However, this high amide-I frequency is consistent with conformational energy calculations of Scheraga and co-workers. The mechanism of the dichloroacetic acid-induced transition to an α-helix is discussed. Dichloroacetic acid and dimethyl sulfoxide interact strongly and the transition presumably involves a marked decrease in the ability of dimethyl sulfoxide to solvate the peptide backbone and aromatic side chains upon complex formation with dichloroacetic acid.     

Non-bonded interatomic potential functions and crystal structure. Correction of the functions for use with macromolecules and application to polypeptide helixes

On the basis of a set of nonbonded interatomic potential functions derived earlier from heats of sublimation and experimental crystal structures, we derive a second, less repulsive, set which is to be used in the absence of the expansion caused by thermal motion and in particular in macromolecular systems where thermal motion is much reduced compared with crystals of small molecules. Working with a pair of octane molecules, we calculate the intermolecular potential (U) in the presence of thermal motion from potentials U° (in the absence of thermal motion), by letting a system of pairs of molecules assume a Boltzmann distribution over the intermolecular distance, in the presence of a force of varied magnitude applied to obtain different equilibrium distances. The potential U° is adjusted until the calculated and the empirical potentials U agree. Finally, best interatomic Lennard-Jones potentials which reproduce the function U° are calculated. The resulting functions are tested by calculating the crystal structure of benzene and comparing it with experimental data at low temperature, by energy minimization of the crystal structure of polyethylene and of the β-structure of poly-L -alanine, and by comparing the energy of the α-helix and the β-structure of poly-L -alanine. In all cases, the corrected functions give more satisfactory results than the uncorrected set.