Vibrational CD of the amide II band in some model polypeptides and proteins.

The amide II vibrational CD (VCD) spectra of poly (L-glutamic acid) and poly (L-lysine) in various conformational forms and those of several proteins in H2O have been measured. Characteristic VCD patterns have been observed in the amide II region due to helix, beta-sheet, and coil conformations in polypeptides. Based on their x-ray crystal structures, the proteins studied have been assigned to six categories. Proteins in the same category give rise to similar amide II VCD. While the protein conformational type is indicated using the amide II VCD, discrimination between types is less characteristic than with the previously studied amide I' VCD in D2O.     

Vibrational circular dichroism spectra of unblocked proline oligomers.

Vibrational Circular Dichroism (VCD) spectra of unblocked L-proline oligopeptides, (Pro)n n = 3 to 7, dissolved in D2O are reported. For these oligomers, the VCD spectra can be attributed to a conformational dominance of the trans amide conformation with subunits interrelated by a left-handed twist, particularly for the longer oligomers. As a function of oligomer length, formation of this conformation starts at n = 3; and by n = 5 a spectrum closely resembling that of the poly-L-proline II helix in shape and magnitude is seen. The VCD data are compared with previous (Pro)n results using IR, CD, Raman and NMR spectroscopies, and reasons for the variations in interpretation are discussed.     

Vibrational circular dichroism spectroscopy of selected oligopeptide conformations

Vibrational circular dichroism (VCD) has been shown to be a useful technique for characterization of the qualitative secondary structure type for linear polypeptides and oligopeptides. A brief review of characteristic spectral responses and applications is given. Since VCD is dependent on relatively short range interactions, it detects residual structure in such oligomers even if long range order is lost. VCD studies presented here for Lys oligomers as well as Lys and Glu polymers as a function of length, salt added and temperature, confirm residual local order in these 'random coils'. Comparison to results with Pro oligomers, supports an interpretation that these extended structures have a left handed twist conformation. The 'coil' VCD is shown to be significantly reduced in intensity by temperature increase and by decrease in peptide length. By contrast, for partially alpha-helical Ac-(AAKAA)3GY-NH2 oligomers, the spectrum changes to the high temperature Lys(n) shape on heating, first losing then gaining intensity, indicating an equilibrium shift between structured states, from helix to coil (locally ordered) forms. VCD is shown to be a useful technique for monitoring local order in otherwise random coil structures.     

Noncovalent interactions of peptides with porphyrins in aqueous solution: conformational study using vibrational CD spectroscopy.

Noncovalent interactions of poly(L-lysine) (PL), oligopeptides L-lysyl-L-alanyl-L-alanine and (L-lysyl-L-alanyl-L-alanine)(2) with meso-tetrakis(4-sulfonatophenyl)porphine (TPPS), and poly(L-glutamic acid) (PLGA) with meso-tetrakis(1-methyl-4-pyridyl)porphine tetra-p-tosylate (TMPyP) in aqueous solutions have been studied using combination of spectroscopic methods: Vibrational circular dichroism (VCD) spectroscopy in the mid-infrared region provides a direct information on conformational changes of the polypeptides and oligopeptides caused by interactions with porphyrins; ultraviolet-visible absorption, fluorescence, and electronic circular dichroism (ECD) reveal the aggregation characterization of the porphyrin part of the complexes. Interactions of TPPS with tripeptide, hexapeptide, and PL containing about ten amino acid residues in the molecular chain are accompanied with the changes of VCD patterns in the amide I' region. In these cases, the conformation of the oligopeptide part of complexes is obviously influenced by interactions with TPPS and partial changes of random coil structure are observed in VCD. When PL was composed of the hundreds of lysine residues, just a weak intensity decrease was detected and the shape of VCD spectrum typical for the random coil structure was preserved. As follows from the uv-vis absorption and fluorescence spectra, porphyrin molecules are attached to peptides by electrostatic interaction as a monomer or dimer and interaction between porphyrin and peptide depends on the polypeptide chain length. For the PLGA-TMPyP system with PLGA containing from tens to hundreds of glutamic acid residues in the chain, the VCD spectra were unchanged when TMPyP was presented in the aqueous solution of PLGA and random coil conformation of PLGA-TMPyP aggregates was preserved.     

Theoretical CD studies of polypeptide helices: examination of important electronic and geometric factors

An improved model for calculating the CD of polypeptides has been developed. Excited state wavefunctions were derived from CNDO/S (complete neglect of differential overlap, spectroscopic) calculations on N-methylacetamide. Four discrete peptide-localized transitions were employed: pi 0 pi* (NV1), pi* + pi* (NV2), n pi*, and n' pi*. Inclusion of the pi + pi transition (lambda 0 = 140 nm) significantly improves the accuracy of the calculated CD spectra in the 180-250-nm region. Spectra were computed for various helical structures, including right-handed alpha-, alpha II-, omega-, pi-, 3(10-), and poly (proline) I-helices, and the left-handed poly (proline) II-helix. Sensitivity to changes in the peptide backbone geometry and chain length are examined. Electronic factors such as ground-state charge distribution, hybridization effects, and basis set deorthogonalization have been investigated. The nonconservative nature of the poly (Pro) I and II CD spectra is reproduced, and the helix band present in earlier exciton calculations on the alpha-helix has been diminished.     

Quantitative IR spectrophotometry of peptide compounds in water (H2O) solutions. II. Amide absorption bands of polypeptides and fibrous proteins in alpha-, beta-, and random coil conformations.

Infrared spectra of poly(D,L-alanine), poly(L-glutamic acid), poly(L-lysine), silk fibroin, and tropomyosin have been registered for various conformations of the polypeptide chain. Assuming additivity of the main- and side-chain absorption, spectral parameters of amide I and II absorption bands corresponding to alpha-, beta-, and random coil conformations have been derived. The amide I band parameters for H2O and D2O have been compared.     

Conformational study of sequential Lys and Leu based polymers and oligomers using vibrational and electronic CD spectra

Vibrational CD (VCD) and electronic CD (ECD) spectra of some sequential Lys and Leu based oligo- and polypeptides were studied as a function of added salt and (for ECD) as a function of concentration in aqueous solution. For these samples, the VCD spectra can only be measured at relatively high concentrations under which the well-known salt-induced transition to a β-sheet form can be observed for the KL based species, but only the end-state α-helical conformation is obvious for the LKKL based samples. ECD concentration dependence demonstrates that, at high concentration with no added or with added salt, LKKL based oligomers and polymers give α-helical spectra. These data provide evidence of aggregation induced secondary structure formation in an exceptionally simple peptide system. Similarly, the KL based oligomers and polymers give β-sheet like spectra at high concentration or at high salt. These systems further provide model systems under “normal” aqueous conditions that yield VCD band shapes that correlate to the major secondary structural types of polypeptides. They are in substantial agreement with those spectra obtained on homopolypeptides and on proteins, confirming the relative independence of the VCD technique from side-chain and solvent effects. © 1994 John Wiley & Sons, Inc.     

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

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

Conformations of alanine-based peptides in water probed by FTIR, Raman, vibrational circular dichroism, electronic circular dichroism, and NMR spectroscopy

We have used a combination of FTIR, VCD, ECD, Raman, and NMR spectroscopies to probe the solution conformations sampled by H-(AAKA)-OH by utilizing an excitonic coupling model and constraints imposed by the 3JCalphaHNH coupling constants of the central residues to simulate the amide I' profile of the IR, isotropic Raman, anisotropic Raman, and VCD spectra in terms of a mixture of three conformations, i.e., polyproline II, beta-strand and right-handed helical. The representative coordinates of the three conformations were obtained from published coil libraries. Alanine was found to exhibit PPII fractions of 0.60 or greater, mixed with smaller fractions of helices and beta-strand conformations. Lysine showed no clear conformational propensity in that it samples polyproline II, beta-strand, and helical conformations with comparable probability. This is at variance with results obtained earlier for ionized polylysine, which suggest a high polyproline II propensity. We reanalyzed previously investigated tetra- and trialanine by combining published vibrational spectroscopy data with 3JCalphaHNH coupling constants and obtained again blends dominated by PPII with smaller admixtures of beta-strand and right-handed helical conformations. The polyproline II propensity of alanine was found to be higher in tetraalanine than in trialanine. For all peptides investigated, our results rule out a substantial population of turn-like conformations. Our results are in excellent agreement with MD simulations on short alanine peptides by Gnanakaran and Garcia [(2003) J. Phys. Chem. B 107, 12555-12557] but at variance with multiple MD simulations particularly for the alanine dipeptide.     

Effects of proline ring conformation on theoretical pi-pi* absorption and CD spectra of helical poly(L-proline) forms I and II

Absorption and CD spectra of the pi-pi* transition near 200 nm are calculated for helical (Pro)10 forms I and II with a variable proline ring conformation characterized by torsion angle chi 2 in the range -60 degrees to 60 degrees. The spectra for poly(Pro) I are not sufficiently sensitive to chi 2 to suggest a preferred ring conformation. The spectra for poly(Pro) II are more sensitive to chi 2, and suggest preferred ring conformations near either or both of the chi 2 regions -50 +/- 10 degrees and 50 +/- 10 degrees.     

Structural composition of betaI- and betaII-proteins

Circular dichroism spectra of proteins are sensitive to protein secondary structure. The CD spectra of alpha-rich proteins are similar to those of model alpha-helices, but beta-rich proteins exhibit CD spectra that are reminiscent of CD spectra of either model beta-sheets or unordered polypeptides. The existence of these two types of CD spectra for beta-rich proteins form the basis for their classification as betaI- and betaII-proteins. Although the conformation of beta-sheets is largely responsible for the CD spectra of betaI-proteins, the source of betaII-protein CD, which resembles that of unordered polypeptides, is not completely understood. The CD spectra of unordered polypeptides are similar to that of the poly(Pro)II helix, and the poly(Pro)II-type (P2) structure forms a significant fraction of the unordered conformation in globular proteins. We have compared the beta-sheet and P2 structure contents in beta-rich proteins to understand the origin of betaII-protein CD. We find that betaII-proteins have a ratio of P2 to beta-sheet content greater than 0.4, whereas for betaI-proteins this ratio is less than 0.4. The beta-sheet content in betaI-proteins is generally higher than that in betaII-proteins. The origin of two classes of CD spectra for beta-rich proteins appears to lie in their relative beta-sheet and P2 structure contents.     

Solution structure of native proteins with irregular folds from Raman optical activity

Raman optical activity (ROA) spectra have been measured for the proteins hen phosvitin, yeast invertase, bovine alpha-casein, soybean Bowman-Birk protease inhibitor, and rabbit Cd(7)-metallothionein, all of which have irregular folds in the native state. The results show that ROA is able to distinguish between two types of disorder. Specifically, invertase, alpha-casein, the Bowman-Birk inhibitor, and metallothionein appear to possess a "static" type of disorder similar to that in disordered states of poly(L-lysine) and poly(L-glutamic acid); whereas phosvitin appears to possess a more "dynamic" type of disorder similar to that in reduced (unfolded) lysozyme and ribonuclease A and also in molten globule protein states. In the delimiting cases, static disorder corresponds to that found in loops and turns within native proteins with well-defined tertiary folds that contain sequences of residues with fixed but nonrepetitive phi,psi angles; and dynamic disorder corresponds to that envisaged for the model random coil in which there is a distribution of Ramachandran phi,psi angles for each amino acid residue, giving rise to an ensemble of interconverting conformers. In both cases there is a propensity for the phi,psi angles to correspond to the alpha, beta and poly(L-proline) II (PPII) regions of the Ramachandran surface, as in native proteins with well-defined tertiary folds. Our results suggest that, with the exception of invertase and metallothionein, an important conformational element present in the polypeptide and protein states supporting the static type of disorder is that of the PPII helix. Long sequences of relatively unconstrained PPII helix, as in alpha-casein, may impart a plastic (rheomorphic) character to the structure.     

IR (vibrational) CD of peptide beta-turns: a theoretical and experimental study of cyclo-(-Gly-Pro-Gly-D-Ala-Pro-).

IR vibrational CD (VCD) has been observed for the cyclic pentapeptide cyclo-(-Gly-Pro-Gly-D-Ala-Pro-) in solution in CDBr3. The observed VCD spectra do not resemble the VCD features of any of the previously reported peptide secondary structures, such as alpha-helical, "random coil," or sheet structures, and might be due to the beta-turn contained in this molecule. To shed light onto the origin of the observed spectra, VCD intensity calculations, based on the solution and solid-state structures of cyclo-(-Gly-Pro-Gly-D-Ala-Pro-), have been carried out. In addition, calculated VCD data for pure beta-turns are discussed.     

Plant prolyl hydroxylase recognizes poly(L-proline) II helix

Substrate specificity of a prolyl hydroxylase from Vinca rosea suspension-cultured cells was studied using synthetic oligo(L-proline)s and their t-butyloxycarbonyl derivatives (Pron and Boc-Pron; n = 2-8) as peptidyl substrates. All peptides with a residual number of 5 or greater served as substrates in the enzyme reaction at 30 degrees C, after the preincubation of the enzyme and peptides at 0 degrees C prior to addition of cofactors and cosubstrate. Under the same conditions, the hydroxylation of Pro5 reached a plateau within 10 min, but that of Boc-Pro8 and poly(L-proline) increased linearly up to 40 min. If the preincubation temperature was raised to 30 degrees C, only Pro5 among the peptides was unable to serve as a substrate. The optimum temperature of the enzyme was 30 degrees C toward Boc-Pro8 and poly(L-proline) but it decreased to 15 degrees C using Pro5. These data suggest that the enzyme can bind Pro5 only at low temperature. Poly(L-proline) and Boc-Pron (n greater than or equal to 5) in aqueous solution are known to have a left-handed helical structure (poly(L-proline) II helix). Moreover, Pro5 was indicated as forming this helix below 10 degrees C. Accordingly, the enzyme recognizes the poly(L-proline) II helix, that is, the secondary structure of a substrate rather than the primary structure.     

Purification and properties of the bifunctional proline dehydrogenase/1-pyrroline-5-carboxylate dehydrogenase from Pseudomonas aeruginosa

Proline dehydrogenase/1-pyrroline-5-carboxylate dehydrogenase (Pro/P5C dehydrogenase), a bifunctional enzyme catalyzing the two consecutive reactions of the oxidation of proline to glutamic acid, was purified from Pseudomonas aeruginosa strain PAO1. Pro/P5C dehydrogenase oxidized L-proline in an FAD-dependent reaction to L-delta 1-pyrroline-5-carboxylic acid and converted this intermediate with NAD or NADP as cosubstrates to L-glutamic acid. The purification procedure involved DEAE-cellulose chromatography, affinity chromatography on Matrex gel red A and gel filtration on Sephadex G-200. It resulted, after 40-fold purification with 11% yield, in a homogeneous preparation (greater than 98% pure). The molecular weight of the single subunit was determined as 119,000. Gel filtration of purified Pro/P5C dehydrogenase yielded a molecular weight of 242,000 while polyacrylamide gel electrophoresis under native conditions led to the appearance of two catalytically active forms of the enzyme with molecular weights of 241,000 and 470,000. Manual Edman degradation revealed proline, alanine and aspartic acid as the N-terminal amino acid sequence. Pro/P5C dehydrogenase was highly specific for the L-forms of proline and delta 1-pyrroline-5-carboxylic acid. Its apparent Km values were 45 mM for L-proline, 0.03 mM for NAD and 0.17 mM for NADP. The saturation function for delta 1-pyrroline-5-carboxylic acid was non-hyperbolic.     

Vibrational circular dichroism of polypeptides. II. Solution amide II and deuteration results

Vibrational CD (VCD) of amide I and II vibrations of several α-helical polypeptides have been measured in solution. For the amide II as well as the amide I [previously published: Lal, B.B. & Nafie, L.A. (1982) Biopolymers 21 , 2161] we find the VCD to be characteristic of the polypeptide secondary structure. Amide II bands of right-handed α helices were all found to have negative VCD and to have their maximum rotational strength for the parallel (low-energy) component. However, left-handed α helices formed from L -amino acids gave positive amide II bands at higher frequencies than found for the right-handed helices, indicating that the VCD was sensitive to the stereochemical difference. The amide-I VCD spectra of some deuterated right-handed α-helical polypeptides have a new negative feature to low frequency that does not reflect theoretical predictions but also appears to be stereochemically sensitive. Amide-II and amide-A VCD of a few deuterated polypeptides imply retention of the secondary-structure-dependent characteristics seen in the hydrogenated VCD.     

Conformational properties of the proline region of porcine neuropeptide Y by CD and 1H-NMR spectroscopy

We synthesized porcine neuropeptide Y (pNPY) N-terminal fragments by solid-phase synthesis techniques and analyzed them for solution Conformational properties by CD and ¹H-nmr spectroscopy. The analogues pNPY_1–9 and pNPY_1–14 displayed CD spectra indicative of random structures and showed no evidence for induced α-helical structures in trifluoroethanol (TFE) up to 50%. However, the CD spectra of pNPY_1-9 suggested a Conformational shift in tetrahydrofuran. Although in aqueous solution the CD spectra of pNPY_1–21 indicated random structures with induction of only a small percentage of α-helix in aqueous TFE, pNPY_1-25 displayed 13% a-helical structure in aqueous solution that increased to 40 and 41% by the addition of TFE and methanol, respectively. The nmr spectra of pNPY_1-9 and the proline region of pNPY_1–25 indicated extended structures with all-trans conformers at Pro5 and Pro8 for pNPY_1–9 and at Pro5, Pro8, and Pro13 for pNPY_1–25; in each case the Tyrl-Pro2 amide bond was in both cis and trans conformations. However, observed nuclear Overhauser effect correlations and UN exchange experiments indicated an α-helical segment in pNPY_1–25 initiated by Pro 13 and extending from residues 14 to 25. Thus, the N-terminal polyproline region of NPY has no propensity to fold into a regular secondary structure, although Pro 13 is a helix initiator, a result consistent with the proposed role of this amino acid in the NPY structural model. © 1995 John Wiley & Sons, Inc.     

Conformational study of linear alternating and mixed D- and L-proline oligomers using electronic and vibrational CD and fourier transform IR

Vibrational CD (VCD) spectra of a series of blocked linear, alternating D - and L -proline containing oligopeptides, dissolved in D₂O and in CDCl₃. are reported. For the Boc-LDL -Pro₃ to Boc-DLDLDLDL-Pro₈ oligomers. The VCD spectra in the amide I band is a positive couplet, opposite in sense to that obtained for (L -Pro)_n oligomers. While this admits the possibility of their favoring a right-handed helical chain conformation, the amide I ir spectra for these dl oligomers in D₂O indicate a mixed, apparently alternate, cis-trans conformation that prevents a simple conclusion. Their VCD in D₂O evidence no narrowing and has a progressive loss in intensity (measured as Δ /A,) with an increase in chain length. In CDCl₃a similar pattern of positive VCD couplets decreasing in intensity with length was seen, but their spectra are narrower. Their electronic CD (ECD) in the uv, also indicates a loss in intensity with increasing length. Oligomers with odd or even numbers of Pro residues have different ECD patterns, indicating that those spectra are strongly influenced by local contributions arising in the N-terminal groups. The VCD arises from dipolar and vibrational coupling of the amides in the helical structure. All the spectra are consistent with the chiral end groups leading to formation of an excess of one helical handedness. With an increase in length, the influence of this selectiveness is less and the overall CD measured decreases. © 1995 John Wiley & Sons, Inc.