Conformation of poly(L-arginine). II. Complexes with polyanions

Conformaitons of poly(L -arginine)/polyanion complexes were studies by CD measurements. The polyanions were the homoplolypeptides poly(L -glutamic acid) and poly(L -aspartic acid); the synthetic polyelectrolytes and polyethylenesulfonate; and the polynucleotides were native DNA, denatured DNA, and poly(U). It was found that poly(L -arginine) forms the α-helical conformation by interacting with the acidic homopolypeptides and the synthetic anionic polyelectrolytes. In each complex, poly(L -glutamic acid) is in the α-helical conformation, whereas poly(L -aspartic acid) is mostly in the random structure. The poly(L -glutamic acid) complex changed into the β-sheet structure at the transition temperature about 65°C in 0.01M cacodylate buffer (pH 7). Even in the presence of 5M urea, this complex remained in the α-helical conformation at room temperature. The existence of the stable complex of α-helical poly(L -arginine) and α-helical poly(L -glutamic acid) was successfully supported by the model building study of the complex. The α-helix of poly(L -arginine) induced by binding with polyacrylate was the most stable of the poly(L -arginine)-polyanion complexes examined as evidenced by thermal and urea effects. The lower helical content of the polyethylenesulfonate-complexed poly(L -aginine) was explained in terms of the higher charge density of the polyanion. On the other hand, native DNA, denatured DNA, and poly(U) were not effective in stabilizing the helical structure of poly(L -arginine). This may be due to the rigidity of polyanions and to the steric hindrance of bases. Furthermore, the distinitive structual behavior of poly(L -arginine) and poly(L -lysine) regarding polyanion interaction has been noticed throughout the study.     

Conformational studies on Cu(II) polycomplexes of pyridoxal Schiff bases of polypeptides

Structures of Cu(II) complexes of pyridoxal Schiff bases with poly(L -lysine), poly(L -ornithine), and poly(L -α,γ-diaminobutyric acid) were investigated by absorption spectra, CD, and conformational analysis. Although the polypeptides retain their typical right-handed α-helical conformation, opposite Cotton effects were found for the poly(L -lysine) and poly(L -ornithine) polycomplexes in the whole range of wavelengths from 600 to 250 nm. As in the analogous derivatives of salicyladehyde, this effect seems to be due to a stereospecific binding of the square planar Cu(II)-bis-pyridoxylideneimine group to the α-helical matrix. Circular dichroism spectrum of poly(L -α,γ-diaminobutyric acid) polycomplex is similar to that found for poly(L -lysine) derivative, but indicates large tetrahedral distortion of the square-planar coordination of copper ion.     

Conformational studies of sequential polypeptides containing lysine and tyrosine

The conformation of three sequential copolypeptides, poly(L -tyrosyl-L -lysine), poly(L -tyrosyl-L -lysyl-L -lysine), and poly[L -tyrosyl-(L -lysyl)₂-L -lysine] have been studied by a variety of techniques, including CD, ir spectroscopy, analytical ultracentrifugation, and x-ray diffraction. Depending upon the pH and sovent composition, poly(L -tyrosyl-L lysyl-L -lysine) and poly [L -tyrosyl-(L lysyl)₂-L -lysine] can adopt either the α-helical or random-coil conformation, while poly(L -tyrosyl-L -lysine) forms either inter- or intramolecular β-structures.     

Conformation of poly(L-homoarginine)

Poly(L -arginine) assumes the α-helix in the presence of the tetrahedral-type anions or some polyanions by forming the “ringed-structure bridge” between guanidinium groups and anions which is stabilized by a pair of hydrogen bonds and electrostatic interaction [Ichimura, S., Mita, K. & Zama, M. (1978) Biopolymers 17 , 2769–2782; Mita, K., Ichimura, S. & Zama, M. (1978) Biopolymers 17 , 2783–2798]. This paper describes the parallel CD studies on the conformational effects on poly (L -homoarginine) of various mono-, di-, polyvalent anions and some polyanions, as well as alcohol and sodium dodecylsulfate. The random coil to α-helix transition of poly(L -homoarginine) occurred only in NaClO₄ solution or in the presence of high content of ethanol or methanol. The divalent and polyvalent anions of the tetrahedral type (SO, HPO, and P₂O), which are strong α-helix-forming agents for poly(L -arginine), failed to induce the α-helical conformation of poly(L -homoarginine). By complexing with poly(L -glutamic acid) or with polyacrylate, which is also a strong α-helix-forming agent for poly(L -arginine), poly(L -homoarginine) only partially formed the α-helical conformation. Monovalent anions (OH^?, Cl^?, F^?, and H₂PO) did not change poly(L -homoarginine) to the α-helix, and in the range of pH 2–11, the polypeptide remained in an unordered conformation. In sodium dodecylsulfate, poly(L -homoarginine) exhibited the remarkably enlarged CD spectrum of an extended conformation, while poly(L -arginine) forms the α-helix by interacting with the agent. Thus poly(L -homoarginine), compared with poly(L -arginine), has a much lower ability to form the α-helical conformation by interacting with anions. The stronger hydrophobicity of homoarginine residue in comparison with the arginine residue would provide unfavorable conditions to maintain the α-helical conformation.     

Anisotropic rotational motions of poly(L-glutamic acid) in the alpha-helix conformation

The anisotropic rotational motion of the backbone and the side chains of poly(L -glutamic acid) in the α-helical structure was investigated using the ¹³C-T₁ and T₂ relaxation times of all carbon atoms with directly attached protons, obtained at a ¹³C-Larmor frequency of 67.89 MHz. The evaluation of the nmr data was carried out according to the previously derived anisotropic diffusion model, in which the macromolecule is considered a rigid rod. The rotation of the backbone is characterized by two diffusion constants, D₁ and D₃, describing the rotation perpendicular to and around the symmetry axis. The additional internal motion of the C^β-methylene group is described as a jump process with a jump rate, k₁, between two allowed rotametric states. Steric considerations indicate that the occupation of the third rotameric position is forbidden. The rotation of the C^γ-methylene group is decribed as a one-dimensional diffusion process around the C^β–C^γ bond. Investigation of the temperature dependence of the relaxation parameters led to the temperature dependence of the dynamic parameters. Activation energies were determined from these data. The dynamic parameters obtained for poly(L -glutamic acid) at 291 K are compared with the corresponding results of a previous study of poly(L -lysine). The development of an anisotropic diffusion model for the motions of the rod-shaped poly(L -lysine) α-helix and its application to the interpretation of the ¹³C-relaxation data of this molecule have already been published previously. In this model, both the overall molecular tumbling and the various internal motions have been characterized by diffusion constants or jump rates typical for each process. These dynamic parameters can be calculated from the spin–lattice relaxation times, the spin–spin relaxation times and the NOE factors of the C^α, C^β, and C^γ nuclei of the polypetide. In the present paper, we describe the application of the above-mentioned dynamic model to the interpretation of ¹³C-relaxation studies of a further homopolypeptide, poly(L -glutamic acid), in the α-helical structure. Furthermore, we studied the temperature dependence of the relaxation times of this polymer and determined the anisotropic diffusion parameters at each temperature. From their temperature dependence and from comparison of our present results with the data of our previous study of poly(L -lysine), we were able to derive new insights into the intramolecular diffusion processes and the excitation of various motions.     

Flow-induced conformational changes and phase behavior of aqueous poly-L-lysine solutions

Poly-L -lysine exists as an α-helix at high pH and a random coil at neutral pH. When the α-helix is heated above 27°C, the macromolecule undergoes a conformational transition to a β-sheet. In this study, the stability of the secondary structure of poly-L -lysine in solutions subjected to shear flow, at temperatures below the α-helix to β-sheet transition temperature, were examined using Raman spectroscopy and CD. Solutions initially in the α-helical state showed time-dependent increases in viscosity with shearing, rising as much as an order of magnitude. Visual observation and turbidity measurements showed the formation of a gel-like phase under flow. Laser Raman measurements demonstrated the presence of small amounts of β-sheet structure evidenced by the amide I band at 1666 cm⁻¹. CD measurements indicated that solutions of predominantly α-helical conformation at 20°C transformed into 85% α-helix and 15% β-sheet after being sheared for 20 min. However, on continued shearing the content of β-sheet conformation decreased. The observed phenomena were explained in terms of a “zipping-up” molecular model based on flow enhanced hydrophobic interactions similar to that observed in gel-forming flexible polymers. © 1998 John Wiley & Sons, Inc. Biopoly 45: 239–246, 1998     

The Interaction of New Pyridylporphyrins with Bovine Serum Albumin

The interaction of meso-tetra(4-N-hydroxyethylpyridyl)porphyrin, meso-tetra(3-N-hydroxyethylpyridyl)porphyrin, and their zinc complexes with bovine serum albumin (BSA) was studied by electronic spectroscopy, CD, and equilibrium dialysis at pH 7.2. The titration of the porphyrins with BSA was accompanied by a decrease in light absorption and a bathochromic shift of the Soret band, as well as by the appearance of an isobestic point. The porphyrin interaction with BSA also led to the induction of positive CD spectra in the visible region, which is explained by the porphyrin sorption on the protein globule. The equilibrium dialysis helped in determining the stoichiometry of binding and the binding constants of the porphyrins under study with BSA using Scatchard plots. This interaction is nonspecific and reversible.     

Poly(L-lysyl-L-alanyl-alpha-L-glutamic acid). II. Conformational studies.

The solution characterization of poly(Lys-Ala-Glu) is described. This polytripeptide is zwitterionic at neutral pH and is shown to take on a conformation which is dictated by the state of ionization, molecular weight, temperature, and solvent. The polypeptide is almost entirely α-helical at low pH and temperature for polymers of greater than 25,000 molecular weight. Melting profiles for these conditions show t_m ～ 20°C. Analysis of circular dichroism curves shows the α-helical content to vary in a linear manner with molecular weight in the range 3000–30,000. At neutral pH the charged polypeptide is essentially random, but substantial α-helix could be induced by addition of methanol or trifluoroethanol. At temperatures where the sequential polypeptide is a random coil, addition of trifluoroethanol produces a polymer which is mostly α-helical but also contains an appreciable ammount of β-structure. The infrared spectrum of a low-molecular-weight fraction assumed to be cyclo(Lys-Ala-Glu)₂ was tentatively assigned a β-pleated sheet structure. A comparison of this polytripeptide in various ionization states with other polytripeptides containing L -alanine and L -glutamate or L -lysine shows the α-helix directing properties for the (uncharged) residues to lie in the order Ala > Glu > Lys.     

Hydrodynamic behavior and molecular conformation of poly(L-lysine HBr) in carbonate buffer solution

In carbonate buffer at pH 10.5, a transparent solution of poly(L -lysine HBr) was obtained up to fairly high concentration of 3 g/dl at room temperature. The hydrodynamic behavior of the solution has been studied by sedimentation analyses and viscosity measurements. A dimer form for high concentrations and a monomer form for low concentrations were inferred. The dimer and monomer forms were assigned to a β-structure and α-helix, respectively, based on the CD and optical rotary dispersion spectra. Using CD spectroscopy, a reversible transition between α-helix and β-structure was observed as a function of either poly(L -lysine HBr) concentration or temperature. An aggregated form which was assigned to the antiparallel pleated sheet appeared at 50°C on the basis of its ir spectrum.     

Vibrational analysis of peptides, polypeptides, and proteins. XXXII. alpha-Poly(L-glutamic acid)

The Raman and ir spectra of α-helical poly(L -glutamic acid) have been assigned on the basis of a normal mode calculation for this structure. The force field was based on our previously refined main-chain force constants for α-poly(L -alanine) and side-chain force constants for β-calcium–poly(L -glutamate). Despite the identical backbone α-helical structures, significantly different frequencies are calculated, and observed, in the amide III and backbone stretch regions of α-poly(L -glutamic acid), as compared with α-poly(L -alanine). This clearly demonstrates the influence of side-chain structure on mainchain vibrational modes.     

Spin-label studies of the pH-induced random coil to α-helix conformational transition in poly(L-lysine)

Poly(L -lysine) of various molecular weights between 2700 and 475,000 was spin-labeled. From the electron spin resonance spectra, the degree of freedom of the nitroxide was determined by calculation of the rotational correlation time as the poly(L -lysine) underwent the pH-induced random coil to α-helix conformational transition. In general, the rotational correlation time of the nitroxide increased as the pH was increased, indicating a more restricted environment for the spin label when poly(L -lysine) is deprotonated. For the high-molecular-weight poly(L -lysine) this corresponds to the formation of the α-helix and indicates that the side chain–side chain interaction and decreased segmental motion of the backbone (slightly) restricts the motion of the spin label. For the 2700-molecular-weight poly(L -lysine), previously shown not to assume a helical conformation at high pH, the increase in the rotational correlation time of the spin label indicates that the side chain–side chain interaction takes place after deprotonation but without helix formation. This may indicate that helix formation per se is not needed to produce the observed effect even with the high-molecular-weight polymers. The rotational correlation time of the spin label at a particular pH did not depend on the molecular weight of the poly(L -lysine) over the 200-fold range of molecular weights. This indicates that the rotational correlation time reflects the rotational mobility of the spin label in a localized environment and not the rotational diffusion of the entire macromolecule.     

Secondary structure of proteins associated in thin films

The solid state secondary structure of myoglobin, RNase A, concanavalin A (Con A), poly(L -lysine), and two linear heterooligomeric peptides were examined by both far-uv CD spectroscopy¹ and by ir spectroscopy. The proteins associated from water solution on glass and mica surfaces into noncrystalline, amorphous films, as judged by transmission electron microscopy of carbon-platinum replicas of surface and cross-fractured layer. The association into the solid state induced insignificant changes in the amide CD spectra of all α-helical myoglobin, decreased the molar ellipticity of the α/β RNase A, and increased the molar ellipticity of all-β Con A with no change in the positions of the bands' maxima. High-temperature exposure of the films induced permanent changes in the conformation of all proteins, resulting in less α-helix and more β-sheet structure. The results suggest that the protein α-helices are less stable in films and that the secondary structure may rearrange into β-sheets at high temperature. Two heterooligomeric peptides and poly (L -lysine), all in solution at neutral pH with “random coil” conformation, formed films with variable degrees of their secondary structure in β-sheets or β-turns. The result corresponded to the protein-derived Chou-Fasman amino acid propensities, and depended on both temperature and solvent used. The ir and CD spectra correlations of the peptides in the solid state indicate that the CD spectrum of a “random” structure in films differs from random coil in solution. Formic acid treatment transformed the secondary structure of the protein and peptide films into a stable α-helix or β-sheet conformations. The results indicate that the proteins aggregate into a noncrystalline, glass-like state with preserved secondary structure. The solid state secondary structure may undergo further irreversible transformations induced by heat or solvent. © 1993 John Wiley & Sons, Inc.     

Circular dichroism of collagen, gelatin, and poly(proline) II in the vacuum ultraviolet.

Circular dichroism spectra for acid-soluble calfskin collagen, gelatin, and poly(proline) II in solution have been extended into the vacuum ultraviolet region. The extended spectrum of gelatin reveals that the circular dichroism of this unordered polymer is more closely related to the spectrum of charged polypeptides than might be evident from near ultraviolet work. A short-wavelength band is found at about 172 nm, which corresponds in position, magnitude, and sign to a band recorded earlier for poly(L -glutamic acid) at pH 8.0. This band is observed in a helical structure for the first time in the vacuum ultraviolet circular dichroism and absorption spectra of poly(proline) II. Both circular dichroism and absorption spectra point to the assignement of this band as the nσ*. Neither the nσ* nor the expected positive lobe of the ππ* helix band is observed in the extended circular dichroism spectrum of collagen. We postulate that these two bands cancel here in analogy to the case of α-helical poly(L -glutamic acid).     

The solution conformation of poly(L-lysine). A Raman and infrared spectroscopic study.

The Raman and infrared spectra of poly(L -lysine) and poly(DL -lysine) in solution are reported and the effects of various salts are investigated. The results demonstrate that α-helix formation in solution is induced by specific salts and the spectral data support the hypothesis of regions of local order for poly(L -lysine) in aqueous solutions of low ionic strength.     

Change in mobility of side chains due to neutralization of charged poly(L-lysine) with dansyl group

Poly(L -lysine) having dansyl (5-dimethylamino-1-naphthalene-sulfonyl) groups to its side chains was prepared. The fluorescence spectra and fluorescence anisotropy ratios of the dansyl (DNS) group were measured in various conditions. In aqueous solution the increase in emission intensity was observed reflecting the alkali-induced coil-to-helix transition. In aqueous-methanolic solutions with methanol content above 60 wt %, the poly(L -lysine) with DNS group (DNS-PLL) was probed to show α-helical conformation from CD spectra. With addition of alkali, the increase in fluorescence intensity of α-helical DNS-PLL and the drastic change in fluorescence anisotropy ratio were observed. In this case the rotational mobility of DNS probe decreases, gives a minimum at a certain concentration of added alkali, and then increases again up to approximately the initial level. At the concentration where the rotational mobility gives the minimum, intensity of scattered light gives a maximum. This shows that suppression of the mobility of DNS side chains is caused by the intermolecular aggregation of α-helical DNS-PLL. This concentration of added alkali corresponds to the midpoint of neutralization to charged side chains of the DNS-PLL. The interaction that causes aggregate of α-helical DNS-PLL is suggested to be the intermolecular hydrogen bonding between neutralized and unneutralized side chains. © 1994 John Wiley & Sons, Inc.     

Conformational studies of polymers and copolymers of L-aspartate ester. II. Infrared studies and the factors involved in the formation of the omega-helix

It has already been show that the helix senses of poly(β-benzyl L -aspartate) and poly(β-methyl L -aspartate) are left-handed, while the poly esters of n-propyl, isopropyl, n-butyl, and phenethyl L -asparate are all right-handed. The effect of changes in helix sense from the left-handed to the right-handed α-helical form on the infrared spectra of copolymers of benzyl L -aspartate with ethyl, n-butyl, isopropyl, n-propyl, and phenethyl L -aspartate have been studied. Those show that for the right-handed helical form the amide band frequencies fall within the range given by Elliott,⁷ while for the left-handed form the frequencies are higher. The frequency ranges for the two helix senses are given and have been used to show that poly (β-n-propyl L -aspartate) in chloroform solution undergoes a transition from the right-handed to the left-handed helix form on heating. Polarized infrared studies of the different copolymers show that the disposition of the side chain ester groups is different for the two forms. Although methyl L -aspartate forms a left-handed α-helix similar to benzyl L -aspartate, the introduction of methyl L -aspartate residues into poly (β-benzyl L -aspartate) prevents the formation of the ω-helix. The factors involved in the formation of this helix form are discussed.     

Photoresponsive polypeptides: Photochromism and conformation of poly (L-glutamic acid) containing spiropyran units

Spirobenzopyran units were bound to the side chains of poly (L -glutamic acid) and partially methylated poly(L -glutamate)s. The modified polymers were found to exhibit “reverse photochromism” in hexafluoro-2-propanol (HFP), so the samples kept in the dark were characterized by an intense absorption band in the visible range of the spectrum, which was completely erased upon exposure to sunlight or irradiation at 500–550 nm. The CD spectra showed that the macromolecules adopted a random coil conformation in the dark, whereas the bleached solutions after exposure to light displayed the typical CD pattern of the α-helix. The back reaction in the dark was accompanied by the progressive decrease of the helix content and recovery of the original disordered conformation. The photoinduced conformational changes resulted in large and reversible viscosity variations. When spiropyran side chains were converted to “spiropyran salts” of trifluoroacetic acid, the system was still photochromic, but the macromolecules were disordered both in the dark and light conditions. However, when appropriate amounts of methanol were added as a cosolvent to the HFP solutions, the system responded to light, giving reversible variations of the α-helix content. Irradiation at appropriate solvent compositions allowed modulation of the extent of the photoresponse. © 1993 John Wiley & Sons, Inc.     

Differentiation between the α-helical and coillike conformations of poly(L-glutamic acid) in aqueous solution through binding of pinacyanol

Pinacyanol in the presence of an excess of poly(L -glutamic acid) [polymer/dye ratio (P/D) > 10] exhibits different absorption spectra in the visible region when bound to the slightly charged polypeptide in the α-helical conformation or to the nearly completely dissociated polypeptide in the coillike conformation. These spectra reveal aggregation of the dye bound to the macromolecular chain in both conformations, although in the coillike one different kinds of aggregates may be present. Dye binding is accompanied by the appearance of CD bands in the visible region which are also different for the α-helical and the coillike conformations. The aggregates formed in the presence of the latter change slowly in time and seem to induce some conformational changes in the polypeptide chain. Furthermore, they have been found to be, at least partially, stable with respect to a subsequent reversal to the α-helical conformation. All results could be qualitatively interpreted assuming that in the coillike conformation, ordered regions exist along the chain as proposed by Krimm and Tiffany.     

Protein conformation in bacterial spinae

The far uv circular dichroism (CD) and infrared spectra of bacterial spinae are reported. Estimates of the protein secondary structure were obtained by three-component curve-fitting methods supplemented by rank and factor analysis of CD data matrices. Native spinae were shown to contain approximately 88% antiparallel β-sheet, 7% α-helix, and 5% unordered structure based on estimates using poly(L -lysine). Basis CD spectra derived from globular proteins were shown to give unreliable estimates.     

Proton magnetic resonance and optical spectroscopic studies of watr-soluble polypeptides: poly-L-lysine HBr, poly(L-glutamic acid), and copoly(L-glutamic acid42, L-lysine HBr28, L-alanine)

The helix-coil transition has been studied by high-resolution NMR for three water-soluble polypeptides. Such systems are better models for protein behavior than those in TFA-CDCl₃ solvent. An upfield shift of ～7 cps is observed for the α-CH peak of poly(L -glutamic acid) and poly-L -lysine as the helix content increases over the transition. No such shift is found for copoly(L -glutamic acid⁴², L -lysine²⁸, L -alanine³⁰). The width of the α-CH peak for poly L-lysine increases rapidly as helix content rises but for poly L -glutamic acid and the copolymer, the width of this peak remains unchanged up to 60% helicity. This demonstrates a rapid rate of interconversion between helical and random conformations in partly helical polymer for the latter two polypeptides. All three polymers however, show no apparent α-CH peak at 100% helicity. Side-chain resonance lines also broaden as helix content increases and, to a greater extent, the closer the proton is to the main chain.