Optical properties of the polyglycine II helix

The circular dichroism spectrum obtained from a dilute aqueous solution of poly (ala-gly-gly) resembles that described for charged polypeptides such as the salt form of poly glutamic acid. A similar spectrum is found for films cast from aqueous solution where x-ray studies reported elsewhere have indicated a poly-glycinc II conformation. Evidence is presented for a heat induced poly-glycine II to unordered state transition similar to that described for collagen. The interpretation of this, the first observation of the optical properties of a poly-amino acid in the poly glycine II conformation, is further rationalized on the basis of spectra obtained from a number of polypeptides whose conformation approaches that of a 3₁ helix.     

Synthesis and characterization of four sequential glycyl/glutamate polypeptides

Poly(Glu(OBzl)-Gly)_n, poly(Glu-Gly)_n, poly(Gly)-(Glu(OBzl)-Gly), and poly(Gly-Glu-Gly) were synthesized from the pentachlorophenyl esters of the sequential monomer. Both of the polymers containing free glumatic-acid residues are soluble in water, as is the lower molecular weight fraction of the polytripeptides with the benzyl ester in place. Circular dichroism studies and infrared dichroism studies suggest that the 2₁ helix is favored for the polydipeptide with removal of the benzyl ester reducing the conformational integrity. The polytripeptide showed evidence of 3₁ helix in addition to the 2₁ form, depending on solvent. A rationale for the conformations observed is developed based on the bulkiness of the side-chain residues and conformational stabilization, in certain cases, by hydrophobic interactions between the benzyl ester groups.     

Characterization of two sequential polytripeptides containing glycine and ethyl-glutamate residues

The polytripeptides poly(glu(OEt)-gly-gly) and poly(glu(OEt)-glu(OEt)-gly) have been synthesized and characterized using infrared linear dichroism, ultraviolet circular dichroism spectroscopy, and electron microscopy. Both polymers have been obtained in a cross β conformation with antiparallel chains, however, there appear to be significant differences in the stability of this conformation for the two polymers. Poly(glu(OEt)-gly-gly) has also been shown to exist in a 3₁ polyglycine II type helix in aqueous solution whereas films cast from this solution appear to be random. Finally this same polymer can be obtained in either a random or an extended form trifluoroacetic acid depending on the nature of the substrate used for film casting.     

Spectroscopic characterization of poly(Glu-Ala)

Infrared linear dichroism and ultraviolet circular dichroism speetroscopy have been used to distinguish four conformational forms of the ionizable sequential polypeptide poly(Glu-Ala). Two of these conformations, the α helix and the β form, were observed for the unionized polypeptide in solution. The α helix appeared immediately upon neutralization of the side-chain carboxyl functions, whereas the β form was observed after the neutralized solution had been standing for several days. The β form was also observed for films cast from either high or low pH solutions. Ionization of the glutamyl residues resulted in a circular dichroism spectrum which has previously been observed for charged homopolymers and appears to result from an extended helical conformation. Further, heating either the α helical or the charged extended helix resulted in a transition to a disordered chain. These results are consistent with the results of conformational calculations presented elsewhere.     

Vibrational circular dichroism spectra of three conformationally distinct states and an unordered state of poly(L-lysine) in deuterated aqueous solution

Fourier transform ir vibrational circular dichroism (VCD) spectra in the amide I′ region of poly(L-lysine) in D₂O solutions have confirmed the existence of three distinct conformational states and an unordered conformational state in this homopolypeptide. Characteristic VCD spectra are presented for the right-handed α-helix, the antiparallel β-sheet, an extended helix conformation previously referred to as the so-called “random coil,” and a completely unordered conformation characterized by the absence of any amide I′ VCD. VCD for the antiparallel β-sheet in solution and the unordered chain conformation are presented for the first time. Each of the four different VCD spectra is unique in appearance and lends weight to the view that VCD has the potential to become a sensitive new probe of the secondary structure of proteins in solution.     

Synthesis and characterization of poly(LysAla3)

The synthesis and characterization of poly(LysAla₃) are described. The polytetrapeptide is a model for short sequences found in proelastin, and is presumably involved in desmosine or isodesmosine cross-link formation in the native protein. Poly(LysAla₃) is found to possess a mixture of conformations in aqueous solution dependent on molecular weight and pH. Low-molecular-weight (ca. 3000) material appears to be a mixture of random and extended helix at neutral pH. However, as the molecular weight is increased an increasing amount of α-helix is observed rising to >50% for mol wt = 21,000. The α-helical chain segments are thermally stable, melting to a mixture of extended and random forms at T_m = 25°C. High pH (10.5) promotes further α-helix formation but at pH >11.0 the polypeptide becomes insoluble. The inference is that short chain segments of the peptide in elastin are unlikely to be α-helical in the equilibrium state but may fluctuate through such a conformation.     

Kinetic studies of the helix–coil transition in aqueous solutions of poly(L-lysine)

The rate of conformational change of aqueous poly(α-L -lysine) solutions was measured using the electric field pulse relaxation method with conductivity detection. The relaxation time as a function of pH exhibits two maxima. One is assigned to a proton transfer reaction and the other to the helix–coil conformational transition. The helix nucleation parameter and the maximum relaxation time yield the rate constant of helix growth process (k_F) according to Schwarz's kinetic theory as k_F = 2 × 10⁷ sec^?1, which is comparable to that of the poly(glutamic acid) solution. The thermodynamic parameters of the helix growth process are compared with those of poly(glutamic acid).     

Theory of melting of the triple helix poly (A + 2U) for a 1 : 2 mixture of Poly A to Poly U

The Zimm-Bragg theory is extended to treat the melting of the triple helix poly (A + 2U) for a solution with a 1 : 2 mole ratio of poly A to poly U. Only the case for long chains is considered. For a given set of parameters the theory predicts the fraction of segments in the triple helix, double helix, and random coil states as a function of temperature. Four nucleation parameters are introduced to describe the two order–disorder transitions (poly (A + 2U) ? poly A + 2 poly U and poly (A + U) ? poly A + poly U) and the single order–order transition (poly (A + 2U) ? poly (A + U) + poly U). A relation between the nucleation parameters is obtained which reduces the number of independent parameters to three. A method for determining these parameters from experiment is presented. From the previously published data of Blake, Massoulié and Fresco⁸ for [Na⁺] = 0.04, we find σ_T = 6.0 × 10^?4, σ_D = 1.0 × 10^?3, and σσ* = 1.5 × 10^?3. σ_T and σ_D are the nucleation parameters for nucleating a triple helix and double helix, respectively, from a random coil region. σσ* is the nucleation parameter for nucleating a triple helix from a double helix and a single strand. Melting curves are generated from the theory and compared with the experimental melting curves.     

Microcalorimetric studies of solvent-induced conformational change of sodium and cesium salts of poly(L-glutamic acid) in aqueous media

Organic solvent-induced coil → helix conformational change of poly(sodium) L -glutamate (NaPLG) and poly(cesium L -glutamate) (CsPLG) in solution in aqueous mixed solvents have been studied at 25°C. Heats of dilution of NaPLG in the water–dioxane pair have been measured as a function of polymer concentration and solvent composition. The results indicate that the overall chain conformation in the disordered form is not too different from that in the α-helical form. Heat capacity measurements by flow microcalorimetry have also been done. The apparent monomolar heat capacity at constant pressure of the polymer, C_{p, ?}, decreases with dilution similarly to other strong polyelectrolytes in aqueous media. In the water–dioxane pair, C_{p, ?} increases with the dioxane content due to partial desolvation of ionic species resulting from increasing ionic association. In the case of the water-2-chloroethanol (CE) pair, the transition takes place at low CE content and results show a fast decrease in C_{p, ?} when the α-helical conformation predominates. It is believed carboxylate groups and CE molecules associate themselves into a complex formation responsible for the transition. The size of the cation plays a significant role in the thermodynamic properties of these polyelectrolytes in solution since sodium ions are more strongly bound to the chain than cesium ions.     

The Structure of Triple Helical Poly(U)·Poly(A)·Poly(U) Studied by Raman Spectroscopy

Abstract

Using Raman spectroscopy, we examined the ribose-phosphate backbone conformation, the hydrogen bonding interactions, and the stacking of the bases of the poly(U)·poly(A) ·poly(U) triple helix. We compared the Raman spectra of poly(U)·poly(A)·poly(U) in H₂O and D₂O with those obtained for single-stranded poly(A) and poly(U) and for double-stranded poly(A)·poly(U). The presence of a Raman band at 863 cm^?1 indicated that the backbone conformations of the two poly(U) chains are different in the triple helix. The sugar conformation of the poly(U) chain held to the poly(A) by Watson-Crick base pairing is C3′ endo; that of the second poly(U) chain may be C2′ endo. Raman hypochromism of the bands associated with base vibrations demonstrated that uracil residues stack to the same extent in double helical poly(A)·poly(U) and in the triple-stranded structure. An increase in the Raman hypochromism of the bands associated with adenine bases indicated that the stacking of adenine residues is greater in the triple helix than in the double helical form. Our data further suggest that the environment of the carbonyls of the uracil residues is different for the different strands.     

Conformational Analysis of the β-amyloid Peptide Fragment, β(12–28)

Abstract

NMR and CD spectroscopy have been used to examine the conformation of the peptide, β(12–28), (VHHQKLVFFAEDVGSNK) in aqueous and 60% TFE/40% H₂0 solution at pH 2.4. In 60% TFE solution, the peptide is helical as confirmed by the CD spectrum and by the pattern of the NOE cross peaks detected in the NOESY spectrum of the peptide. In aqueous solution, the peptide adopts a more extended and flexible conformation. Broadening of resonances at low temperature, temperature-dependent changes in the chemical shifts of several of the CH_α resonances and the observation of a number of NOE contacts between the hydrophobic side-chain protons of the peptide are indicative of aggregation in aqueous solution. The behavior of β(12–28) in 60% TFE and in aqueous solution are consistent with the overall conformation and aggregation behavior reported for the larger peptide fragment, β(1–28) and the parent β-amyloid peptide.     

1H-nmr comparative studies of polynucleotides: Conformation and dynamic structure of polyribo(uridylic) and polyribo(cytidylic) acids in neutral solution

The conformation and the dynamic structure of single-stranded poly(U) and poly(C) in neutral aqueous solution have been investigated by ¹H-nmr at two different frequencies (90 and 250 MHz) and at various temperatures. Measurements of proton chemical shifts, coupling constants J_H-H, and proton relaxation times, T₁, T₂, versus temperature show a striking difference in conformation and in dynamic structure between the two polynucleotides studied. The temperature effect on δ and J_H-H is found to be substantial for poly(C) and insignificant for poly(U). The S conformer is favored in poly(U), whereas the N conformer strongly predominates in poly(C) (?90%), similar to the case for RNAs. These results suggest that single-stranded poly(C) probably possesses a helical or partial helical structure, whereas poly(U) shows a clear preference for the random coil, in agreement with the optical results. The local motions of the ribose and base were studied at various temperatures by measurements on the relaxation times at 90 and 250 MHz. For a given temperature between 22 and 72°C, the ratio T₁(90)/T₁(250) is practically the same for all poly(U) protons, indicating that in this temperature interval the ribose base unit of poly(U) undergoes an isotropic motion characterized by a single correlation time τ_c. Above 52°C, poly(C) exhibits a dynamic structure similar to poly(U). Below this temperature, poly(C) exists in an equilibrium between randomly coiled and single-stranded helix forms. This situation is characterized by a strong cross-relaxation effect and T₁ values corresponding to a relatively short apparent correlation time. An activation energy of 4 kcal/mol was determined for the motion of the ribose–base unit in both single-stranded polynucleotides.     

Folding and assembly of TMD 6‐related segments of DMT 1 in trifluoroethanol aqueous solution

Divalent metal‐ion transporter 1 (DMT1) belongs to a large class of metal‐ion transporters that drive the translocation of a wide range of divalent metal substrates across membranes toward the cytosol with couple of protons. Two highly conserved histidines in the sixth transmembrane domain (TMD6) are essential for metal transport activity in DMT1. In the present study, we determine the high‐resolution structures of three 25‐residue peptides, corresponding to TMD6 of the wildtype DMT1 (the segment 255–279) and its H267A and H272A mutants, in 30% TFE‐d₂ aqueous solution by the combined use of circular dichroism (CD) and NMR spectroscopies. The wildtype peptide forms an ‘α‐helix‐extended segment‐α‐helix’ structure with two helices spanning over Gly258–Ala262 and Met265–Lys277 linked by a hinge at residues Val263–Ile264. The H267A mutation reduces the hinge to one residue (Ile264), while the H272A mutation extends the flexible region of the central part from Val263 to His267. Diffusion‐ordered spectroscopy (DOSY) study demonstrates that all the peptides are self‐assembly as trimer in 30% TFE‐d₂ aqueous solution. The H272A substitution decreases the intermolecular interaction whereas the H267A substitution may enhance the intermolecular interaction. The specific structure of the discontinuous helix and the self‐assembly feature of DMT1–TMD6 may be crucial for its biological function. The changes in conformation and intermolecular interaction induced by histidine substitution may be correlated with the deficiency of DMT1 in metal‐ion permeation. Copyright © 2011 European Peptide Society and John Wiley & Sons, Ltd.     

Alternative conformations of DNA modified by N-2-acetylaminofluorene

Modification of DNA by the carcinogen N-acetoxy-N-2-acetylaminofluorene gives two adducts, a major one at the C-8 position of guanine and a minor one at the N-2 position with differing conformations. Binding at the C-8 position results in a large distortion of the DNA helix referred to as the “base displacement model” with the carcinogen inserted into the DNA helix and the guanosine displaced to the outside. The result is increased susceptibility to nuclease S, digestion due to the presence of large, single-stranded regions in the modified DNA. In contrast, the N-2 adduct results in much less distortion of the helix and is less susceptible to nuclease S₁ digestion. A third and predominant adduct is formed in vivo, the deacetylated C-8 guanine adduct. The conformation of this adduct has been investigated using the dimer dApdG as a model for DNA. The attachment of aminofluorene (AF) residues introduced smaller changes in the circular dichroism (CD) spectra of dApdG than binding of acetylaminofluorene (AAF) residues. Similarly, binding of AF residues caused lower upfield shifts for the H-2 and H-8 protons of adenine than the AAF residues. These results suggest that AF residues are less stacked with neighboring bases than AAF and induce less distortion in conformation of the modified regions than AAF. An alternative conformation of AAF-modified deoxyguanosine has been suggested based on studies of poly(dG-dC)·poly(dG-dC). Modification of this copolymer with AAF to an extent of 28% showed a CD spectrum that had the characteristics of the left-handed Z conformation seen in unmodified poly-(dG-dC)·poly(dG-dC) at high ethanol or salt concentrations. Poly(dG)·poly(dC), which docs not undergo the B to Z transition at high ethanol concentrations, did not show this type of conformational change with high AAF modification. Differences in conformation were suggested by single-strand specific nuclease S₁ digestion and reactivity with anticytidine antibodies. Highly modified poly(dG-dC)·poly(dG-dC) was almost completely resistant to nuclease S₁ hydrolysis, while, modified DNA and poly(dG)·poly(dC) are highly susceptible to digestion. Two possible conformations for deoxyguanosine modified at the C-8 position by AAF are compared depending on whether its position is in alternating purine-pyrimidine sequences or random sequence DNA.     

Conformation and aggregation of melittin: effect of pH and concentration of sodium dodecyl sulfate

The conformation of melittin, a surface-active polypeptide, in solution was studied by CD spectra between 190 and 240 nm. The molecule was essentially unordered (possibly with a trace of helix) in water without salt at neutral pH. Upon deprotonation of four of the six cationic groups at pH 12 the polypeptide became partially helical (about 35%). The addition of NaDodSO₄ to an aqueous melittin solution first caused the solution to become turbid but it became clear again in excess surfactant solution. The conformational changes depended on the molar NaDodSO₄/melittin ratio, R. With R from 2.34 to 23.4, the melittin solution was turbid and the polypeptide conformation was probably a mixture of α-helix and β-sheets. This was supported by the ir spectrum of the turbid solution, which indicated the presence of both conformations. With R = 46.8 or 468 (1 or 10 mM NaDodSO₄) the polypeptide conformation was characteristic of an α-helix, about 70–80% of the molecule, regardless of whether the surfactant was above or below its critical micelle concentration. This compared well with the x-ray results of 92% helix in crystals. The lower helicity of melittin in NaDodSO₄ solution might be attributed to the end effects that destabilize the first and last turn of an helix at its N- and C-terminus, respectively.     

Salt-induced extension and dissociation of a native double-stranded xanthan

This study shows that xanthan molecules at room temperature may assume at least three different conformations in 0.1 m NaCl aqueous solutions in which the local structure is ordered: (1) the native compact double helix, (2) the extended double helix, and (3) the extended single helix. Experiments including viscosity, low-angle light scattering and optical rotation measurements have been carried out with a fully pyruvated and fully acetylated native laboratory sample supplied as fermentation broth. Two major conformation changes of the native double helix which were found irreversible in our experimental conditions can be induced by treatments at low ionic strength. After treatment in 10⁻⁴m NaCl, xanthan is still a double helix in 10⁻¹m NaCl, but the backbone of each strand has been extended. After the sample has been in 10⁻⁵m NaCl, the double helix has been dissociated and a single helix sample is obtained. Thus, the denaturing of xanthan is a two-step process. The first step consists of the extension of the two chains inside the double helix, and the second is a dissociation of the native double strand.     

Spectroscopic studies on the structure of poly(8-bromoadenylic acid): Effect of glycosidic torsion angle on the conformation and flexibility in polyribonucleotides

The helix–coil transition and conformational structure of poly(8-bromoadenylic acid) [poly(8BrA)] have been investigated using ¹H- and ¹³C-nmr, CD, and ir spectroscopy. The results have been compared with the structure of the related 5′-mono- and polynucleotides. The chemical shifts of H(2′), H(3′), C(2′), and C(3′) nmr signals show an interesting correlation with both the puckering of ribose ring and glycosidic bond torsion angle. Poly(8BrA) shows an upfield shift of the C(3′) signal and a downfield shift of the H(3′) signal compared to the chemical shifts in poly(A). These shifts are consistent with a C(3′) endo-syn conformation for poly(8BrA). A similar effect has been reported previously and is also observed here on the C(2′) and H(2′) signals when the preferred conformation is C(2′)endo-syn (e.g., in 5′-8BrAMP). The chemical-shift parameters thus act as a probe for studying syn ? anti and N ? S equilibria in solutions. The three-bond ¹H-′¹³C coupling constants between H(1′) and C(8) and C(4) have been measured in poly(8BrA) and 5′-8BrAMP and their structural implications have been discussed. The observed preference of a C(3′)endo-syn conformation for poly(8BrA), coupled with other evidence, throws doubt on the validity of a correlation previously reported whereby a syn conformation is associated with a C(2′)endo ribose pucker. The backbone conformation of randomly coiled poly(8BrA) is very similar to the structures found in polyribonucleotides: poly(A) and poly(U). All three polymers show strong preferences for the backbone angles found in RNA helices. The CD spectrum of poly(8BrA) has a striking relationship to that of poly(A). The signs of all extrema are inverted, and the magnitudes are related by a constant factor. We suggest that these differences result from a change in the angle between coupled transition moment vectors in the two polymers. Infrared spectra of poly(8BrA) in H₂O and D₂O solution are reported for the frequency range below 1400 cm^?1. The antisymmetric >PO stretching vibration is observed at an unusually low frequency in the helix (1214 cm^?1). The symmetric >PO stretch occurs at ～1095 cm^?1 but is not resolved from a ring vibration near this frequency. A conformationally sensitive band, characteristic of helical RNA structures, is observed at 817 cm^?1 and disappears when the helix is melted. This observation confirms the conclusion that ordered poly(8BrA) has a regular helical structure with an RNA backbone conformation. A stereochemical explanation is provided for the failure of poly(8BrA) (or other syn polymers) to form double helices with anti-polyribonucleotides.     

Tat cell-penetrating peptide has the characteristics of a poly(proline) II helix in aqueous solution and in SDS micelles.

Tat cell-penetrating peptide (GRKKRRQRRRPPQG) is able to translocate and carry molecules across cell membranes. Using CD spectroscopy the conformation of this synthetic peptide was studied in aqueous and membrane-mimicking, micellar SDS solutions at different temperatures. The CD spectrum of the Tat cell-penetrating peptide in SDS micellar solution was virtually unchanged from that in aqueous solution, and at low temperature it was close to that of a poly(proline) II helix.     

Interactions of mono spermine porphyrin derivative with DNAs

In this work, we have characterized the interactions of monospermine porphyrin derivative with calf thymus DNA (ct-DNA) and poly (dG-dC)₂ in both B and Z conformation. By several spectroscopic techniques (UV–vis, electronic circular dichroism and resonance light scattering), the binding modes of monospermine porphyrin derivative with different DNA sequences have been elucidated. In the presence of ct-DNA, the porphyrin binds along the external double helix as well as in the presence of B conformation of poly (dG-dC)₂. Whilst when the Z form of the poly (dG-dC)₂ is induced, a slight intercalation of the porphyrin between the basis has been detected.     

Solution conformation of an immunogenic peptide from HRV2: comparison with the conformation found in a complex with a Fab fragment of an anti-HRV2 neutralizing antibody

The conformation of a [15]-peptide (H-VKAETRLNPDLQPTE-NH₂) from VP2 of rhinovirus HRV2 complexed with a Fab fragment was previously shown by X-ray crystallographic studies to be similar to the one found in the corresponding region of HRV1A. Antibodies raised against this peptide bind to and neutralize HRV2. In order to identify structural features preserved in solution that may explain the ability of this short peptide to mimic the structure of the protein surface, the peptide has been studied by NMR in aqueous solution as well as under denaturing conditions. The peptide is shown to be a random coil in solution. However, the sequence forming a 3₁₀ helix in the complex is biased into a helical conformation according to NOE intensity data as well as from urea and pH titrations. This sequence adopts the same conformation in an unrelated protein. NOE data suggest that a β-turn found in the complex may be sampled in solution. Also, Glu4, interacting with Arg6 in the crystal, has a reduced pK_a value in solution. It is concluded that the local structure present in the random coil state of VP2(156–170) contains enough information to direct the production of antibodies that bind to and neutralize HRV2. © 1998 European Peptide Society and John Wiley & Sons, Ltd.