Vibrational analysis of peptides,polypeptides, and proteins. VI. Assignment of β-turn modes in insulin and other proteins

The normal modes have been calculated for structures having the dihedral angles of the four β-turns of insulin. Frequencies are predicted in the amide I region near 1652 and 1680 cm^?1. The former overlaps the α-helix band at 1658 cm^?1 in the Raman spectrum, while the latter accounts for the hitherto unassignable band at 1681 cm^?1. Calculated amide III frequencies extend above 1300 cm^?1, providing a compelling assignment of the 1303-cm^?1 band in insulin and similar bands in other globular proteins.     

Laser-excited raman spectroscopy of biomolecules. XII. Thermally induced conformational changes in poly(L-glutamic acid)

The α-helical from of poly(L -glutamic acid) [α-poly(Glu)] gives rise to the same amide I and III lines as α-poly(γ-benzyl-L -glutamate) at 1652 and 1296 cm^?1, respectively. The latter is a superposition of the amide III line near 1290 cm^?1 and a line deu to vibrational made of CH₂ groups of the side chain near 1300 cm^?1. A line at 924 cm^?1 is tentatively identified as characteristics of α-poly(Glu). Both the β₁- and β₂- forms of poly(Glu) give rise to characteristic of β-amide. III frequencies that are similar because of their similar backbone structures. Differences in the conformations of their side chains and in the environments of the backbone are reflected in the region 800–1200 cm^?1 and in the amide I. A line at 1042 cm^?1 and a pair at 1021 and 1059 cm^?1 are tentatively assigned as characteristic of β₁-poly(Glu) and β₂-poly(Glu), respectively. The α-β₂ transition in poly(L -Glu⁷⁸L -Val²²) is shown by the appearance of all the β₂-characteristic lines in the thermally transformed sample. The same features observed in poly(L -Glu⁹⁵L -Val⁵) also indicate that the α-β₂ transition of poly(Glu) is facilitated by the presence of L -valine and that the content of L -valine is not critical for this purpose. Investigation of the Raman spectra of the calcium, strontium, barium and sodium slats of poly(Glu) shows that these salts, under the conditions of preparation used, all the have random-coil conformations.     

Effect of Mid-infrared Free-Electron Laser Irradiation on Refolding of Amyloid-Like Fibrils of Lysozyme into Native Form

Aggregation of lysozyme in an acidic solution generates inactive amyloid-like fibrils, with a broad infrared peak appearing at 1,610?C1,630?cm^?1, characteristic of a ??-sheet rich structure. We report here that spontaneous refolding of these fibrils in water could be promoted by mid-infrared free-electron laser (mid-IR FEL) irradiation targeting the amide bands. The Fourier transform infrared spectrum of the fibrils reflected a ??-sheet content that was as low as that of the native structure, following FEL irradiation at 1,620?cm^?1 (amide I band); both transmission-electron microscopy imaging and Congo Red assay results also demonstrated a reduced fibril structure, and the enzymatic activity of lysozyme fibrils recovered to 70?C90?% of the native form. Both irradiations at 1,535?cm^?1(amide II band) and 1,240?cm^?1 (amide III band) were also more effective for the refolding of the fibrils than mere heating in the absence of FEL. On the contrary, either irradiation at 1,100 or 2,000?cm^?1 afforded only about 60?% recovery of lysozyme activity. These results indicate that the specific FEL irradiation tuned to amide bands is efficient in refolding of lysozyme fibrils into native form.     

Stoichiometry and Preferential Interaction: Two Components of the Principle for Protein Structure Organization

Abstract

The effect of pressure on the conformational structure of amyloid β (1–40) peptide (Aβ(1–40)), exacerbated with or without temperature, was determined by Fourier transform infrared (FT-IR) microspectroscopy. The result indicates the shift of the maximum peak of amide I band of intact solid Aβ(1–40) from 1655 cm^?1 (α-helix) to 1647–1643 cm^?1 (random coil) with the increase of the mechanical pressure. A new peak at 1634 cm^?1 assigned to β-antipar- allel sheet structure was also evident. Furthermore, the peak at 1540 cm^?1 also shifted to 1527 (1529) cm^?1 in amide II band. The former was assigned to the combination of α-helix and random coil structures, and the latter was due to β-sheet structure. Changes in the composition of each component in the deconvoluted and curve-fitted amide I band of the compressed Aβ(1–40) samples were obtained from 33% to 22% for α-helix/random coil structures and from 47% to 57% for β-sheet structure with the increase of pressure, respectively. This demonstrates that pressure might induce the conformational transition from α-helix to random coil and to β-sheet structure. The structural transformation of the compressed Aβ(1–40) samples was synergistically influenced by the combined effects of pressure and temperature. The thermal-induced formation of β-sheet structure was significantly dependent on the pressures applied. The smaller the pressure applied the faster the β-sheet structure transformed. The thermal-dependent transition temperatures of solid Aβ(1–40) prepared by different pressures were near 55–60 °C.     

Laser Raman scattering of cobramine B, a basic protein from cobra venom

Cobramine B, a small basic protein from cobra venom, is selected as a model for studying the scattering intensity of tyrosyl ring vibrations in the Raman spectra of proteins. All three tyrosines in this protein appear to be “buried” in the interior of the molecule and probably involved in interactions which are similar to those of the three “buried” tyrosines in RNase A when it is dissolved in water. Spectral evidence is presented and discussed. The Raman spectra in the 300–1800 cm^?1 region of cobramine B in the solid and solution are compared quantitatively. Several differences exist between the two spectra and may be interpreted in terms of difference in conformation. In the amide I region, a strong single line was observed at 1672 cm^?1 both in the solid and solution spectra, suggesting that this protein may contain a large fraction of antiparallel-β structure. This is supported by the presence of a line at 1235 cm^?1 in the amide III region, which is also characteristic of β-structure. The resolved peaks at 1254 and 1270 cm^?1 indicate the coexistence of some hydrogen-bonded random-coil and some α-helix with the β-structure.     

Infrared spectra of outer and cytoplasmic membranes of Escherichia coli

Outer and cytoplasmic membranes of Escherichia coli were prepared by a method based on isopyenic centrifugation on a sucrose gradient. The infrared spectra of solid films of these membranes were studied. The cytoplasmic membrane had an amide I band at 1657 cm^?1 and an amide II band at 1548 cm^?1. The outer membrane had a broad amide I band at 1631–1657 cm^?1 and an amid II band at 1548 cm^?1 with a shoulder at 1520–1530 cm^?1. Upon deuteration, the amide I band of the cytoplasmic membrane shifted to 1648 cm^?1, whereas the band at 1631 cm^?1 of the outer membrane remained unchanged. After extraction of lipids with chloroform and methanol, the infrared spectra in the amide I and amide II regions of both membranes remained unchanged. Although the outer membrane specifically contained lipopolysaccharide, this could not account for the difference in the infrared spectra of outer and cytoplasmic membranes. It is concluded that a large portion of proteins in the outer membrane is a β-structured polypeptide, while this conformation is found less, if at all in the cytoplasmic membrane.     

A resonance Raman study on the interaction of rifampicin with Escherichia coli RNA polymerase

The technique of resonance Raman spectroscopy has been used to investigate the interaction of the antibiotic rifampicin with Escherichia coli RNA polymerase. Spectra were analyzed by generating the first derivative of each recorded spectrum using the Savitsky-Golay algorithm. The only band that shifted significantly in the resonance Raman spectrum of rifampicin upon the formation of the drug-core polymerase complex was the amide III band. It underwent an 8 cm^?1 shift from 1306 cm^?1 in aqueous solution to 1314 cm^?1. A comparable shift was observed for the rifampicin-holoenzyme complex. Thus, the interaction of the sigma subunit with the core polymerase does not significantly alter the manner in which rifampicin interacts with RNA polymerase. The nature of this shift has been analyzed further by recording the resonance Raman spectrum of rifampicin in a variety of solvents with different hydrogen-bonding ability. In non-hydrogen-bonding solvents (benzene and carbon disulfide) the amide III band was observed at approximately 1220 cm^?1; in dimethyl sulfoxide, a weak hydrogen-bond acceptor, 1274 cm^?1; in water, a strong hydrogen-bonding solvent, 1306 cm^?1; and finally, in triethylamine, a stronger hydrogen-bonding solvent than water, it was observed at 1314 cm^?1. Thus, as the hydrogen-bonding ability of the solvent increased, the amide III band shifted to higher frequency. Based on these results, the rifampicin binding site in RNA polymerase provides a stronger hydrogen-bonding environment for the amidic proton of rifampicin than is encountered when rifampicin is free in aqueous solution.     

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.     

Computer analyses of characteristic infrared bands of globular proteins.

Infrared spectra of myoglobin, ribonuclease, lysozyme, α-chymotrypsin, α-lactalbumin, and β-lactoglobulin A were obtained in deuterium oxide solution in units of absorbance versus wavenumber from 1340 to 1750 cm^?1. The spectra were resolved into Gaussian components by means of an iterative computer program. Resolved characteristic absorption peaks for the two infrared active amide I′ components of antiparallel chain-pleated sheets (β-structure) were obtained. The characteristic amide I′ peaks of α-helical regions and apparently unordered regions overlap in D₂O solution. Absorptivity values for the resolved β-structure peak around 1630 cm^?1 were estimated on the basis of the known structure of ribonuclease, lysozyme, and β-chymotrypsin. The β-structure content of β-lactoglobulin was estimated to be ca. 48% of α-lactalbumin ca. 18%, and of α_s-casein close to zero. The results are in general agreement with conclusions drawn from circular dichroism and optical rotatory dispersion studies.     

Raman spectroscopic study of poly (β-benzyl-L-aspartate) and sequential polypeptides

Poly-β-benzyl-L -aspartate (poly[Asp(OBzl)]) forms either a lefthanded α-helix, β-sheet, ω-helix, or random coil under appropriate conditions. In this paper the Raman spectra of the above poly[Asp(OBzl)] conformations are compared. The Raman active amide I line shifts from 1663 cm^?1 to 1679 cm^?1 upon thermal conversion of poly[Asp(OBzl)] from the α-helical to β-sheet conformation while an intense line appearing at 890 cm^?1 in the spectrum of the α-helix decreases in intensity. The 890 cm^?1 line also displays weak intensity when the polymer is dissolved in chloroform–dichloroacetic acid solution and therefore is converted to the random coil. This line probably arises from a skeletal vibration and is expected to be conformationally sensitive. Similar behavior in the intensity of skeletal vibrations is discussed for other polypeptides undergoing conformational transitions. The Raman spectra of two cross-β-sheet copolypeptides, poly(Ala-Gly) and poly(Ser-Gly), are examined. These sequential polypeptides are model compounds for the crystalline regions of Bombyx mori silk fibroin which forms an extensive β-sheet structure. The amide I, III, and skeletal vibrations appeared in the Raman spectra of these polypeptides at the frequencies and intensities associated with β-sheet homopolypeptides. Since the sequential copolypeptides are intermediate in complexity between the homopolypeptides and the proteins, these results indicate that Raman structure–frequency correlations obtained from homopolypeptide studies can now be applied to protein spectra with greater confidence. The perturbation scheme developed by Krimm and Abe for explaining the frequency splitting of the amide I vibrations in β-sheet polyglycine is applied to poly(L -valine), poly-(Ala-Gly), poly(Ser-Gly), and poly[Asp(OBzl)]. The value of the “unperturbed” frequency, V₀, for poly[Asp(OBzl)] was significantly greater than the corresponding values for the other polypeptides. A structural origin for this difference may be displacement of adjacent hydrogen-bonded chains relative to the standard β-sheet conformation.     

A laser Raman study of lysozyme denaturation

The Raman spectrum of chemically denatured lysozyme was studied. The denaturants studied included dimethyl sulfoxide, LiBr, guanidine · HCl, sodium dodecyl sulfate, and urea. Previous studies have shown that the amide I and amide III regions of the Raman spectrum are sensitive to the nature of the hydrogen bond involving the amide group. The intensity of the amide III band at 1260 cm^?1 (assigned to strongly hydrogen-bonded α-helix structure) relative to the intensity of the amide III band near 1240 cm^?1 (assigned to less strongly hydrogen-bonded groups) is used as a parameter for comparison with other physical parameters used to assess denaturation. The correlation between this Raman parameter and denaturation as evidenced by enzyme activity and viscosity measurements is good, leading to the conclusion that the amide III Raman spectrum is useful for assessing the degree of denaturation. The Raman spectrum clearly depends on the type of denaturant employed, suggesting that there is not one unique denatured state for lysozyme. The data, as interpreted, place constraints on the possible models for lysozyme denaturation. One of these is that the simple two-state model does not seem consistent with the observed Raman spectral changes.     

Low-frequency infrared bands and chain conformations of polypeptides

Infrared spectra of polypeptides were measured in the region of 1800–400 cm^?1. For the α-helical form, disordered form, and antiparallel-chain β-form, amide V band- arising from N-H out-of-plane bending models were observed at 610–620, around 650, and 700–705 cm^?1, respectively, and amide V′ bands arising from N-D out-of-plane bending modes were observed at 455–465, around 510, and a 515–530 cm^?1, respectively. These correlations are useful for conformation diagnoses, particularly for copolyamino-acids or proteins which are not oriented. The nature of low-frequency amide bands are discussed with reference to potential energy distributions calculated for the α-helical form and β form.     

Determination of secondary structure of normal fibrin from human peripheral blood

The secondary structure of human fibrin from normal donors and from bovine and suilline plasma was studied by Fourier transform ir spectroscopy and a quantitative analysis of its secondary structure was suggested. For this purpose, a previously experimented spectrum deconvolution procedure based on the use of the Conjugate Gradient Minimisation Algorithm with the addition of suitable constraints was applied to the analysis of conformation-sensitive amide bands. This procedure was applied to amide I and III analysis of bovine and suilline fibrin, obtained industrially, and to amide III analysis of human fibrin clots. The analysis of both amide I and III in the first case was useful in order to test the reliability of the method. We found bovine, suilline, and human fibrin to contain about 30% α-helix (amide I and III components at 1653 cm⁻¹, and 1312 and 1284 cm⁻¹, respectively), 40% β-sheets (amide I and III components at 1625 and 1231 cm⁻¹, respectively) and 30% turns (amide I and III components at 1696, 1680, 1675 cm⁻¹, and 1249 cm⁻¹, respectively). The precision of the quantitative determination depends on the amount of these structures in the protein. Particularly, the coefficient of variation is < 10% for percentage values of amide I and III components > 15 and 5%, respectively. The good agreement of our quantitative data, obtained separately by amide I and amide III analysis, and consistent with a previous fibrinogen (from commercial sources) study that reports only information about fibrin β-sheet content obtained by factor analysis, leads us to believe that the amounts of secondary structures found (α-helix, β-sheets, and turns) are accurate. © 1997 John Wiley & Sons, Inc. Biopoly 41: 545–553, 1997.     

Raman studies of the crystalline, solution, and alkaline-denatured states of beta-lactoglobulin.

The Raman spectra of β-lactoglobulin in the crystalline, freeze-dried, and solution states are compared. The spectra of the freeze-dried and crystalline proteins were practically identical. The conformationally sensitive amide III line appearing at 1242 cm^?1 increased in intensity 30% upon dissolution of the protein in water which is interpreted as a conformational change in the disordered chains of the protein. This result appears to be a phenomenon for globular proteins containing a large disordered chain fraction. The alkaline denaturation of β-lactoglobulin was studied. When the pH was increased from 6.0 to 11.0, the amide III line shifted from 1242 to 1246 cm^?1, broadened, and decreased in intensity. This is consistent with the conversion of β-sheet regions in β-lactoglobulin to the disordered conformation, as has been proposed by other investigators. At pH 13.5 the amide III shifts to 1257 cm^?1 characteristic of a completely disordered protein, indicating that any remaining “core” of β-sheet has been randomized. Several changes in the intensities of the tyrosine and tryptophan vibrations accompany the denaturation. As the pH is increased from 6.0 (native state) to 11.0 (denatured state) the intensity ratio of two tyrosine ring vibrations, I₈₅₅ cm^?1/I₈₃₀ cm^?1, decreases from 1.0:0.9 to 1.0:1.3. The same ratio for a copolymer consisting of 95% glutamic acid and 5% tyrosine at pH 7.0, where the polymer forms a random coil exposing the tyrosine to the aqueous environment, is 1.0:0.62. This ratio more closely resembles that corresponding to β-lactoglobulin at pH 6.0 (native state) than pH 11.0 (denatured state) suggesting that the average tyrosine in the denatured state may be in a more hydrophobic environment than in the native state. A time-dependent polymerization of the denatured protein reported by other investigators and observed by us may account for the change in the tyrosine environment. A tryptophan vibration appearing at 833 cm^?1 in the spectrum of the native state becomes weak as the pH is increased to 11.0. The intensity of this line may also reflect the local environment of the tryptophan residue.     

Vibrational spectroscopic analysis of LD-sequential, bacterial cell wall peptides: an IR and Raman study

The synthetic, zwitterionic bacterial cell wall peptides—D -Glu^γ-L-Lys, D -Glu^γ-L-Lys-D -Ala, D -Glu^γ-L-Lys-D -Ala-D -Ala, and L-Ala-D -Glu^γ-L-Lys-D -Ala-D -Ala—have been investigated in the crystalline and aqueous solution state applying ir and Raman spectroscopy. Additionally, aqueous solutions of the tetra- and pentapeptide have been investigated by CD spectroscopic techniques. Apart from the dipeptide, whose spectral features were dominated by end-group vibrations, the corresponding ir and Raman active bands of the crystalline peptides in the amide and skeletal regions were found at similar wave numbers, thus suggesting an analogous three-dimensional structure of these compounds. Dominant amide A, I, II, and III bands near 3275, 1630, 1540, and 1220–1250 cm^?1, respectively, in the ir are interpreted in favor of an intermolecularly hydrogen-bonded, β-like structure. The absence of any amide components near 1680–1690 cm^?1, together with the presence of strong amide bands near 1630 cm^?1, and weak bands near 1660 cm^?1 in the ir, which, conversely, were found in the Raman spectra as weak and strong bands, but at corresponding wave numbers, is taken as strong evidence for the presence of the unusual, parallel-arranged β-structure. On the basis of comparative theoretical considerations, a parallel-arranged, “β-type ring” conformation [P. De Santis, S. Morosetti, and R. Rizzo (1974) Macromolecules 7 , 52–58] is hypothesized. The solubilized peptides exhibited distinct similarities with their crystalline counterparts in respect to frequency values and relative intensities of the corresponding ir and Raman-active amide I/I′ components, and of some Raman bands in the skeletal region. This is interpreted in terms of residual short-range order, persisting even in aqueous solution. We concluded that the peptides show a strong propensity to form hydrated, strongly associated aggregates in water. On the basis of amide I/I′ band positions, stable, intramolecular interactions via the amide groups are discarded for the solubilized peptides. Complementarily, the CD data obtained suggest the presence of weakly bent, “open-turn”-like structures for the tetra- and pentapeptide in aqueous solution.     

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.     

Intensities and other spectral parameters of infrared amide bands of polypeptides in the alpha-helical form

Intensities and other spectral parameters of infrared amide I and II bands of α-helical polypeptides in solutions have been determined for poly(γ-benzylglutamate), poly(γ-ethylglutamate), and polymethionine in chloroform, polylysine, poly(glutamic acid), and fibrillar protein tropomyosin from rabbit muscles in heavy water. The majority of spectral parameters are characteristic. The half-width of the amide I band was found to vary in the range of 15–40 cm^?1 for different polypeptides in the different solutions. The correlation between this parameter of the amide I band and the stability of the α-helix was estimated. A new weak band near 1537 cm^?1 of unknown origin was observed for the hydrogen form of polypeptides in the α-helical state.     

The Raman spectra of Bence-Jones proteins. Disulfide stretching frequencies and dependence of Raman intensity of tryptophan residues on their environments

The Raman spectra of Bence-Jones proteins (BJP) were measured for their native and denatured states. All of the native BJPs investigated gave amide I at 1670–1675 cm^?1 and amide III at 1242–1246 cm^?1. Although the amide I was shifted to 1667 cm^?1 upon the LiBr, acid, and thermal denaturation, as expected, the amide III frequency was unaltered, indicating that the antiparallel β- and disordered structures of BJP provide amide III at almost the same frequencies. The intensity of the 880-cm^?1 line of native BJP was relatively intense compared with that of amino acid mixed solution in which the mole ratios of Trp, Phe, and Tyr were adjusted to reproduce the corresponding ratios of BJP. However, the intensity was evidently reduced upon LiBr, acid, and thermal denaturation, approaching that of the amino acid mixture. Thus, the intensity of the 880-cm^?1 line is proposed as a practical probe for the environment of Trp residues. The pH dependence of the intensity of the 880-cm^?1 line suggests that one of two buried Trp residues is exposed between pH 4 and 3.2 and the other between pH 3.2 and 1.4. The variable fragment (V_L) of BJP (Tod) exhibited a S? S stretching Raman line at 525 cm^?1. Provided that the crystallographic data of the V_L of BJP is applicable to V_L of BJP (Tod), the 525 cm^?1 of the S? S stretching frequency should be assigned to a TGG conformation of linkage, but not to the AGT or AGG conformation. This supports Sugeta's model rather than Scheraga's model.     

Laser Raman spectroscopic analysis of angiotensin peptides' conformation

In this study we examined the conformation and side chain environments of angiotensins I, II, III, and [Sar¹-Ile⁵-Ala⁸]angiotensin II using laser Raman spectroscopy. The positions of the amide I bands for all four peptides were found between 1664 and 1673 cm^?1. D₂O exchange studies confirmed the positions of the amide I and amide III bands. The positions of the amide I bands for all the angiotensins were found at approximately 1665 cm^?1 and the amide III bands were all located between 1265 and 1278 cm^?1. From the positions and intensities of the amide I and III bands we concluded that all peptides share the same overall conformation consisting of β-turn structure. Spectral analysis indicated that although the spectra for all the peptides were qualitatively identical there was evidence that the angiotensin conformations were more flexible in the aqueous phase than the solid phase. Examination of the $\text{850}\text{830}$ cm^?1 tyrosine doublet suggested that the tyrosine residue in the peptides is exposed to the solvent environment and becomes more exposed as the peptide length is decreased. Therefore, there are some localized conformational differences among the angiotensins. The conformational data yielded by this study leads us to conclude that the various biological properties ascribed to the angiotensins are not due to different conformations of the peptides. The biological differences could perhaps be attributed to localized interactions of the individual amino acid residues with themselves and with the hormone receptors.     

Raman spectral changes induced by side-chain interactions in racemic poly-gamma-benzyl glutamate

Laser Raman spectra are reported for solid films cast from a series of solutions containing mixtures of right- and left-handed α-helices of poly-γ-benzyl-L - and D -glutamate. Procedures were established for producing spectra that were reproducible in position to ±0.3 cm^?1 and in relative intensity to a few percent for features of interest. Spectra for the pure L and pure D polymers were identical, as expected. Several small but definite spectral changes appear in the mixtures, reaching a maximum for the racemic 50:50 mixture. The changes are a shift of ?1.4 cm^?1 in the amide I peak at 1650.5 cm^?1; a shift of about ?5 cm^?1 in the partially resolved amide III peak at 1291 cm^?1; a shift of +2.5 cm^?1 in the benzyl peak at 3062.5 cm^?1; changes in relative intensity of as much as 50% in several regions; and the marked enhancement of several peaks, particularly that at 254 cm^?1. These changes are discussed in terms of side-chain interactions in the packing of right- and left-handed helices.