A UV resonance Raman investigation of poly(rI): Evidence for cation-dependent structural perturbations

Poly(rI) stabilized by either Na⁺ or K⁺ was investigated using uv resonance Raman (UVRR) spectroscopy. Raman excitation profiles of inosine 5′-monophosphate demonstrated the 250 nm excitation selectively enhances base stacking interactions, while ribose and carbonyl stretching vibrations are preferentially enhanced with 210 nm excitation. These wavelengths were used to examine the structure of poly(rI) in the presence of either K⁺ or Na⁺ as a function of temperature. UVRR studies revealed that the K⁺ stabilized form is more thermally stable, yielding a T_m of ∼ 47°C compared to a T_m of ∼ 30°C for the Na⁺ stabilized form. We observed that both the ribosyl conformation and the coordination of the carbonyl groups depend on the nature of the cation. The C₆O stretching frequency indicates that Na⁺ coordinates much more strongly to the carbonyl groups than K⁺ (1672 cm⁻¹ Na⁺ vs 1684 cm⁻¹ K⁺ at 4°C). Conformationally sensitive modes of the phosphate backbone and the ribosyl ring indicate that Na⁺ stabilized poly(rI) predominantly exists in a C_3′-endo ribose conformation, whereas K⁺ stabilized poly(rI) adopts a C_2′-endo conformation possibly as a consequence of the larger ionic radius of the K⁺ ion. © 1998 John Wiley & Sons, Inc. Biopoly 46: 475–487, 1998     

Crystal-state 3D-structural characterization of novel 3(10)-helical peptides.

The crystal-state conformations of two octapeptides, pBrBz-(D-Iva)8-OtBu (8I) and Ac-[L-(alphaMe)Val]8-OH (8II), the heptapeptide Z-[L-(alphaMe)Val]7-OH (7), the hexapeptide Z-[L-(alphaMe)Leu]6-OtBu (6) and the tetrapeptide alkylamide Z-(Aib)2-L-Glu(OMe)-L-Ala-L-Lol (5) were assessed by x-ray diffraction analyses. Two independent molecules are observed in the asymmetric unit of each L-(alphaMe)Val homo-peptide. All four homo-peptides are folded in a regular 3(10)-helical structure (only the C-terminal H-bonded conformation of the D-Iva octapeptide is distorted to a type-I beta-turn). The hydroxyl groups of the C-terminal carboxyl moieties of the two L-(alphaMe)Val homo-peptides participate in an oxy-analogue of the type-III beta-turn conformation. While the two L-(alphaMe)Val 3(10)-helices are right-handed, the D-Iva and L-(alphaMe)Leu helices are left-handed. The tetrapeptide alkylamide is 3(10)-helical at the N-terminus, but it is mixed 3(10)/alpha-helical at the C-terminus.     

Thermal stability of dehydrophenylalanine-containing model peptides as probed by infrared spectroscopy: a case study of an alpha-helical and a 3(10)-helical peptide

The temperature-dependent secondary-structural changes in the two known helical model peptides Boc-Val-deltaPhe-Ala-Leu-Gly-OMe (1; alpha-helical) and Boc-Leu-Phe-Ala-deltaPhe-Leu-OMe (2; 3(10)-helical), which both comprise a single dehydrophenylalanine (deltaPhe) residue, were investigated by means of FT-IR spectroscopy (peptide film on KBr). Both the first-order and the better-resolved second-order derivative IR spectra of 1 and 2 were analyzed. The nu(NH) (3240-3340 cm(-1)), the Amide-I (1600-1700 cm(-1)), and the Amide-II (1510-1580 cm(-1)) regions of 1 and 2 showed significant differences in thermal-denaturation experiments (22 degrees --> 144 degrees), with the 3(10)-helical peptide (2) being considerably more stable. This observation was rationalized by different patterns and strengths of intramolecular H-bonds, and was qualitatively related to the different geometries of the peptides. Also, a fair degree of residual secondary-structural elements were found even in the 'denatured' states above 104 degrees (1) or 134 degrees (2).     

UV resonance Raman and circular dichroism studies of a DNA duplex containing an A(3)T(3) tract: evidence for a premelting transition and three-centered H-bonds.

The presence of A(n) and A(n)T(n) tracts in double-helical sequences perturbs the structural properties of DNA molecules, resulting in the formation of an alternate conformation to standard B-DNA known as B'-DNA. Evidence for a transition occurring prior to duplex melting in molecules containing A(n) tracts was previously detected by circular dichroism (CD) and calorimetric studies. This premelting transition was attributed to a conformational change from B'- to B-DNA. Structural features of A(n) and A(n)T(n) tracts revealed by X-ray crystallography include a large degree of propeller twisting of adenine bases, narrowed minor grooves, and the formation of three-centered H-bonds between dA and dT bases. We report UV resonance Raman (UVRR) and CD spectroscopic studies of two related DNA dodecamer duplexes, d(CGCAAATTTGCG)(2) (A(3)T(3)) and d(CGCATATATGCG)(2) [(AT)(3)]. These studies address the presence of three-centered H-bonds in the B' conformation and gauge the impact of these putative H-bonds on the structural and thermodynamic properties of the A(3)T(3) duplex. UVRR and CD spectra reveal that the premelting transition is only observed for the A(3)T(3) duplex, is primarily localized to the dA and dT bases, and is associated with base stacking interactions. Spectroscopic changes associated with the premelting transition are not readily detectable for the sugar-phosphate backbone or the cytosine and guanosine bases. The temperature-dependent concerted frequency shifts of dA exocyclic NH(2) and dT C4=O vibrational modes suggest that the A(3)T(3) duplex forms three-centered hydrogen bonds at low temperatures, while the (AT)(3) duplex does not. The enthalpy of this H-bond, estimated from the thermally induced frequency shift of the dT C4=O vibrational mode, is approximately 1.9 kJ/mol or 0.46 kcal/mol.     

Time-resolved UV resonance Raman investigation of protein folding using a rapid mixer: characterization of kinetic folding intermediates of apomyoglobin

The 244-nm excited transient UV resonance Raman spectra are observed for the refolding intermediates of horse apomyoglobin (h-apoMb) with a newly constructed mixed flow cell system, and the results are interpreted on the basis of the spectra observed for the equilibrium acid unfolding of the same protein. The dead time of mixing, which was determined with the appearance of UV Raman bands of imidazolium upon mixing of imidazole with acid, was 150 micros under the flow rate that was adopted. The pH-jump experiments of h-apoMb from pH 2.2 to 5.6 conducted with this device demonstrated the presence of three folding intermediates. On the basis of the analysis of W3 and W7 bands of Trp7 and Trp14, the first intermediate, formed before 250 micros, involved incorporation of Trp14 into the alpha-helix from a random coil. The frequency shift of the W3 band of Trp14 observed for this process was reproduced with a model peptide of the A helix when it forms the alpha-helix. In the second intermediate, formed around 1 ms after the start of refolding, the surroundings of both Trp7 and Trp14 were significantly hydrophobic, suggesting the formation of the hydrophobic core. In the third intermediate appearing around 3 ms, the hydrophobicity was relaxed to the same level as that of the pH 4 equilibrium intermediate, which was investigated in detail with the stationary state technique. The change from the third intermediate to the native state needs more time than 40 ms, while the appearance of the native spectrum after the mixing of the same solutions was confirmed separately.     

Energy landscape of a peptide consisting of alpha-helix, 3(10)-helix, beta-turn, beta-hairpin, and other disordered conformations

The energy landscape of a peptide [Ace-Lys-Gln-Cys-Arg-Glu-Arg-Ala-Nme] in explicit water was studied with a multicanonical molecular dynamics simulation, and the AMBER parm96 force field was used for the energy calculation. The peptide was taken from the recognition helix of the DNA-binding protein, c-MYB: A rugged energy landscape was obtained, in which the random-coil conformations were dominant at room temperature. The CD spectra of the synthesized peptide revealed that it is in the random state at room temperature. However, the 300 K canonical ensemble, Q(300K), contained alpha-helix, 3(10)-helix, beta-turn, and beta-hairpin structures with small but notable probabilities of existence. The complete alpha-helix, imperfect alpha-helix, and random-coil conformations were separated from one another in the conformational space. This means that the peptide must overcome energy barriers to form the alpha-helix. The overcoming process may correspond to the hydrogen-bond rearrangements from peptide-water to peptide-peptide interactions. The beta-turn, imperfect 3(10)-helix, and beta-hairpin structures, among which there are no energy barriers at 300 K, were embedded in the ensemble of the random-coil conformations. Two types of beta-hairpin with different beta-turn regions were observed in Q(300K). The two beta-hairpin structures may have different mechanisms for the beta-hairpin formation. The current study proposes a scheme that the random state of this peptide consists of both ordered and disordered conformations. In contrast, the energy landscape obtained from the parm94 force field was funnel like, in which the peptide formed the helical conformation at room temperature and random coil at high temperature.     

Antiamoebin I in methanol solution: rapid exchange between right-handed and left-handed 3(10)-helical conformations

Antiamoebin I (Aam-I) is a membrane-active peptaibol antibiotic isolated from fungal species belonging to the genera Cephalosporium, Emericellopsis, Gliocladium, and Stilbella. Antiamoebin I has the amino acid sequence: Ac-Phe(1)-Aib-Aib-Aib-Iva-Gly-Leu-Aib(8)-Aib-Hyp-Gln-Iva-Hyp-Aib-Pro-Phl(16). By using the uniformly (13)C,(15)N-labeled sample of Aam-I, the set of conformationally dependent J couplings and (3h)J(NC) couplings through H-bonds were measured. Analysis of these data along with the data on magnetic nonequivalence of the (13)C(beta) nuclei (Deltadelta((13)C(beta))) in Aib and Iva residues allowed us to draw the univocal conclusion that the N-terminal part (Phe(1)-Gly(6)) of Aam-I in MeOH solution is in fast exchange between the right-handed and left-handed 3(10)-helical conformations, with an approximately equal population of both states. An additional conformational exchange process was found at the Aib(8) residue. The (15)N-NMR-relaxation and CD-spectroscopy measurements confirmed these findings. Molecular modeling and Monte Carlo simulations revealed that both exchange processes are correlated and coupled with significant hinge-bending motions around the Aib(8) residue. Our results explain relatively low activity of Aam-I with respect to other 15-amino acid residue peptaibols (for example, zervamicin) in functional and biological tests. The high dynamic 'propensity' possibly prevents both initial binding of the antiamoebin to the membrane and subsequent formation of stable ionic channels according to the barrel-stave mechanism.     

Assignment of the 1511 cm(-1) UV resonance Raman marker band of hemoglobin to tryptophan

New UV resonance Raman (UVRR) data provide convincing evidence that a characteristic 1511 cm(-1) band in the T - R difference spectra of hemoglobin is due to the overtone of the Trp W18 fundamental at 756 cm(-1). Measured isotope shifts for 2-H and 15-N substitution at the indole NH group are twice as large for the 1511 cm(-1) band as for W18, and the 1511 cm(-1) intensity scales with that of W18 in the difference spectrum. Moreover, the UVRR excitation profile of the 1511 cm(-1) band tracks that of another tryptophan band, W16. Both are redshifted in hemoglobin, relative to aqueous tryptophan, reflecting H bonding within a hydrophobic environment in the protein. The 2xW18 assignment had been thrown into question by the observation of remnant 1511 cm(-1) intensity in the T - R spectra of hemoglobin labeled with tryptophan-d(5), a substitution that shifts W18 over 50 cm(-1). However, reexamination of the data suggests that this remnant intensity may result from a subtraction artifact arising from the downshift of another difference band, W3, from 1549 cm(-1) in unlabeled protein to 1522 cm(-1) in labeled protein. Restoration of the 2xW18 assignment establishes that the 1511 cm(-1) difference band, which is a useful indicator of the extent of T-state formation in hemoglobin, arises from the same residue, Trpbeta37, that gives rise to essentially all of the T - R signal from tryptophan.     

Chromophore interactions in flavocytochrome c552: a resonance Raman investigation

Resonance Raman spectra with both Soret and visible excitation have been obtained for Chromatium flavocytochrome c552 and its isolated diheme subunit under varying conditions of pH and inhibitor binding. The spectra are generally consistent with previously established classification schemes for porphyrin ring vibrations. The presence of covalently bound flavin in the protein was apparent in the fluorescent background it produced and in flavin-mediated photoeffects observed in heme Raman spectra obtained at high laser power. No flavin modes were present in the Raman spectra, nor was any evidence of direct heme-flavin interaction found by using this technique; however, a systematic perturbation of heme B1g vibrational frequencies was found in the oxidized holoprotein. The heme vibrational frequencies of c552 are compared to those of the diheme peptide and of other c-type cytochromes. They are consistent with an interpretation that involves pH-dependent changes in axial ligation and treats the hemes and flavin as isolated chromphores communicating via protein-mediated interactions.     

Kinetics of exchangeable protons in Z DNA: a UV resonance Raman study.

We have studied the hydrogen-deuterium exchange kinetics of the exchangeable protons of the poly(dG-dC).poly(dG-dC) in the Z form of the polymer, using resonance Raman spectroscopy with 257 nm and 284 nm excitation wavelengths. In our experimental conditions (4.5 M NaCl, phosphate buffer pH7, 2 degrees C) the two amino protons and the imino proton of guanine are exchanged with the same exchange half-time of 13 min, whereas the two amino protons of cytosine are exchanged with the same exchange half-time of 51 min.     

The rough energy landscape of superfolder GFP is linked to the chromophore

Many green fluorescent protein (GFP) variants have been developed for use as fluorescent tags, and recently a superfolder GFP (sfGFP) has been developed as a robust folding reporter. This new variant shows increased stability and improved folding kinetics, as well as 100% recovery of native protein after denaturation. Here, we characterize sfGFP, and find that this variant exhibits hysteresis as unfolding and refolding equilibrium titration curves are non-coincident even after equilibration for more than eight half-lives as estimated from kinetic unfolding and refolding studies. This hysteresis is attributed to trapping in a native-like intermediate state. Mutational studies directed towards inhibiting chromophore formation indicate that the novel backbone cyclization is responsible for the hysteresis observed in equilibrium titrations of sfGFP. Slow equilibration and the presence of intermediates imply a rough landscape. However, de novo folding in the absence of the chromophore is dominated by a smoother energy landscape than that sampled during unfolding and refolding of the post-translationally modified polypeptide.     

Crystal and molecular structure of Boc-D-Ala-delta Phe-Gly-delta Phe- D-Ala-OMe: a 3 10-helical dehydropeptide

The crystal and molecular structure of the pentapeptide Boc-D-Ala-delta Phe-Gly-delta Phe-D-Ala-OMe, containing two dehydrophenylalanine residues, was determined by x-ray diffraction. The molecule crystallizes in the orthorombic P2(1)2(1)2(1) space group, with a = 10.439(3), b = 15.319(3) and c = 21.099(4) A. In the solid state, the conformation of the pentapeptide is characterized by the presence of two type III' beta-turns. Thus the peptide assumes a left-handed 3(10-helical conformation, the left sense being due to the D configuration of the alanine residues. The two unsaturated residues are located in the (i + 1) position of the first beta-turn and in the (i + 2) position of the second beta-turn, respectively. In the crystal, the helical molecules are linked head to tail by hydrogen bonds. Lateral hydrogen bonds are also formed between molecules related by a twofold screw symmetry. This gives rise to a typical mode of packing characterized by infinite helical "chains,' similar to the packing found in other oligopeptides that adopt a 3(10)-helical structure.     

Design of peptides with alpha,beta-dehydro-residues: synthesis, and crystal and molecular structure of a 3(10)-helical tetrapeptide Boc-L-Val-deltaPhe-deltaPhe-L-Ile-OCH3.

The peptide Boc-L-Val-deltaPhe-deltaPhe-L-Ile-OCH3 was synthesized using the azlactone method in the solution phase, and its crystal and molecular structures were determined by X-ray diffraction. Single crystals were grown by slow evaporation from solution in methanol at 25 degrees C. The crystals belong to an orthorhombic space group P2(1)2(1)2(1) with a = 12.882(7) A, b = 15.430(5) A, c = 18.330(5) A and Z = 4. The structure was determined by direct methods and refined by a least-squares procedure to an R-value of 0.073. The peptide adopts a right-handed 3(10)-helical conformation with backbone torsion angles: phi1 = 56.0(6)degrees, psi1 = -38.0(6)degrees, phi2 = -53.8(6)degrees, psi2 = 23.6(6)degrees, phi3 = -82.9(6)degrees, psi3 = -10.6(7)degrees, phi4 = 124.9(5)degrees. All the peptide bonds are trans. The conformation is stabilized by intramolecular 4-->1 hydrogen bonds involving Boc carbonyl oxygen and NH of deltaPhe3 and CO of Val1 and NH of Ile4. It is noteworthy that the two other chemically very similar peptides: Boc-Val-deltaPhe-deltaPhe-Ala-OCH3 (i) and Boc-Val-deltaPhe-deltaPhe-Val-OCH3 (ii) with differences only at the fourth position have been found to adopt folded conformations with two overlapping beta-turns of types II and III', respectively, whereas the present peptide adopts two overlapping beta-turns of type III. Thus the introduction of Ile at fourth position in a sequence Val-deltaPhe-deltaPhe-X results in the formation of a 3(10)-helix. The crystal structure is stabilized by intermolecular hydrogen bonds involving NH of Val1 and carbonyl oxygen of a symmetry related (-x, y - 1/2, 1/2 + z) deltaPhe2 and NH of deltaPhe2 with carbonyl oxygen of a symmetry related (x, y1/2, 1/2 + z) Ile4. This gives rise to long columns of helical molecules linked head to tail running along [010] direction.     

Nuclear magnetic resonance investigation of lysine–oligopeptides and a complex with d(pA)3pGpC(pT)3

We report proton magnetic resonance studies of a series of lysine oligopeptides in H₂O solution. At pH 5 the protonated ε-amino groups are seen as broad resonances; the peptide NH proton resonances are split by spin–spin coupling with the C^α-H proton, and appear at positions which depend on position in the chain and on chain length. Assignments were made by the europium shift method, and we observed the expected effect of catalysis by the terminal —NH₃⁺ of exchange of the adjacent peptide NH. Coupling constants and the temperature coefficient of chemical shift values were consistent with a non-hydrogen-bonded structure for the oligolysines. The rate and mechanism of NH hydrogen exchange were investigated by line-broadening measurements of the peptide protons as a function of pH. Exchange was found to be OH^? catalyzed, with large differences in the rate depending on position in the chain. Preliminary studies of the complex between double-helical d(pA)₃pGpC(pT)₃ and tetra(L -lysine) were performed using ¹H- and ³¹P-nmr techniques. Pmr spectra of the complex at pH values ranging from 3.98 to 8.15 showed very complicated patterns. Downfield shifts and reduction in exchange rates were observed for several tetra(L -lysine) protons. ³¹P-nmr spectra of the complex reveal an upfield shift of 1 ppm for 3′-5′ phosphate diester resonances on complexation. ³¹P T₁ relaxation times change little on complex formation at low temperature but are altered at higher temperature.     

Structure and energy landscape of a photoswitchable peptide: a replica exchange molecular dynamics study

A replica exchange molecular dynamics (REMD) simulation of a bicyclic azobenzene peptide in explicit dimethyl sulfoxide solution is presented in order to characterize the conformational structures and energy landscape of a photoswitchable peptide. It is shown that an enhanced-sampling technique such as the REMD method is essential to obtain a converged conformational sampling of the peptide at room temperature. This is because conventional MD simulations of less than approximately 100-ns length are either trapped in local minima (at 295 K) or-if run at high temperature-do not resemble the room-temperature REMD results. Calculating various nuclear Overhauser effects (NOEs) and (3)J-couplings, a good overall agreement between the REMD simulations and the NMR experiments of Renner et al. (Biopolymers 2000;54:501-514) is found. In particular, the REMD study confirms the general picture drawn by Renner et al. that the trans-isomer of the azobenzene peptide exhibits a well-defined structure, while the cis-isomer is a conformational heterogeneous system; that is, the trans-isomer occurs in 2 well-defined conformers, while the cis-isomer represents an energetically frustrated system that leads to an ensemble of conformational structures. Employing a principal component analysis of the REMD data, the free energy landscape of the systems is studied at various temperatures. The implications for the folding and unfolding pathways of the system are discussed.     

Intermediacy of poly(L-proline) II and beta-strand conformations in poly(L-lysine) beta-sheet formation probed by temperature-jump/UV resonance Raman spectroscopy

Ultraviolet resonance Raman spectroscopy (UVRR) in combination with a nanosecond temperature jump (T-jump) was used to investigate early steps in the temperature-induced alpha-helix to beta-sheet conformational transition of poly(L-lysine) [poly(K)]. Excitation at 197 nm from a tunable frequency-quadrupled Ti:sapphire laser provided high-quality UVRR spectra, containing multiple conformation-sensitive amide bands. Although un-ionized poly(K) (pH 11.6) is mainly alpha-helical below 30 degrees C, there is a detectable fraction (approximately 15%) of unfolded polypeptide, which is mainly in the poly(L-proline) II (PPII) conformation. However, deviations from the expected amide I and II signals indicate an additional conformation, suggested to be beta-strand. Above 30 degrees C un-ionized poly(K) forms a beta-sheet at a rate (minutes) which increases with increasing temperature. A 22-44 degrees C T-jump is accompanied by prompt amide I and II difference signals suggested to arise from a rapid shift in the PPII/beta-strand equilibrium. These signals are superimposed on a subsequently evolving difference spectrum which is characteristic of PPII, although the extent of conversion is low, approximately 2% at the 3 micros time limit of the experiment. The rise time of the PPII signals is approximately 250 ns, consistent with melting of short alpha-helical segments. A model is proposed in which the melted PPII segments interconvert with beta-strand conformation, whose association through interstrand H-bonding nucleates the formation of beta-sheet. The intrinsic propensity for beta-strand formation could be a determinant of beta-sheet induction time, with implications for the onset of amyloid diseases.     

Hen egg white lysozyme fibrillation: a deep‐UV resonance Raman spectroscopic study

Amyloid fibrils are associated with numerous degenerative diseases. The molecular mechanism of the structural transformation of native protein to the highly ordered cross‐β structure, the key feature of amyloid fibrils, is under active investigation. Conventional biophysical methods have limited application in addressing the problem because of the heterogeneous nature of the system. In this study, we demonstrated that deep‐UV resonance Raman (DUVRR) spectroscopy in combination with circular dichroism (CD) and intrinsic tryptophan fluorescence allowed for quantitative characterization of protein structural evolution at all stages of hen egg white lysozyme fibrillation in vitro. DUVRR spectroscopy was found to be complimentary to the far‐UV CD because it is (i) more sensitive to β ‐sheet than to α ‐helix, and (ii) capable of characterizing quantitatively inhomogeneous and highly light‐scattering samples. In addition, phenylalanine, a natural DUVRR spectroscopic biomarker of protein structural rearrangements, exhibited substantial changes in the Raman cross section of the 1000‐cm^–1 band at various stages of fibrillation. (© 2008 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)