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.     

Solvent effects on the orientation of naphthalene rings in the side chain of poly-gamma-1-naphthylmethyl-L-glutamate

The orientation of naphthalene rings in the side chain of poly-γ-1-naphthylmethyl-L -glutamate (PNLG) in mixed solvents of dichoroethane (DCE) and hexafluoroisopropanol (HFIP) has been studied together with its conformation by infrared, circular dichroism, and fluorescence spectra. The CD pattern of PNLG varies with the solvent composition while it maintains the α-helical conformation. The fluorescence spectra of PNLG in solution show excimer emission of the naphthalene chromophores. The ratio of intensity of the excimer emission to that of the normal fluorescence decreases as the HFIP component in the solvent increases. It is suggested that the naphthalene rings in the side chain of α-helical PNLG are more rigidly orientated in the solvents of higher HFIP ratio.     

Neurophysin-neurohypophyseal hormone interactions: studies using a dansylated vasotocin analogue.

We have synthesized a neurohypophyseal hormone analogue containing an extrinsic fluorescence probe by linking a dansyl (DNS) group to the epsilon-amino group of the lysine at residue 8 of vasotocin. The fluorescence properties of this analogue have been characterized by steady-state and time-resolved spectroscopic methods and compared with those of epsilon-DNS-lysine and the dansylated carboxyl terminal tripeptide Pro-Lys(DNS)-GlyNH2. The binding of this hormone analogue to purified isoforms of bovine neurophysins, the natural carrier proteins of the neurohypophyseal hormones, results in changes in several fluorescence parameters of the dansyl probe. These changes include an increase in intensity and average lifetime, a shift of the emission band to higher energies, and an increase in the emission anisotropy. Anisotropy changes have been used to determine dissociation constants for binding to these neurophysin isoforms. Based on the changes in the fluorescence properties of the dansyl probe, the dansyl group itself interacts with the protein. The degree of the dansyl-neurophysin interaction, however, appears to be different for the full sequence isoform of neurophysin I and the Val89 isoform of neurophysin II.     

多肽的α螺旋结构对多肽与钙调蛋白亲合力的影响

本文设计并采用固相法合成了4种钙调蛋白可结合多肽,这些多肽分成两组,每一组中两个多肽的碱性和疏水性相近,但形成α螺旋结构的倾向(预测)不同。研究了这些多肽与钙调蛋白的相互作用,在Ca~(2+)存在下,这些多肽与丹磺酰钙调蛋白结合,使丹磺酰钙调蛋白的荧光光谱发生显著变化,测定了多肽与钙调蛋白所形成的复合物的解离常数。结果表明,预测形成α螺旋结构倾向较大的多肽与钙调蛋白的亲合力也较大。     

The application of surface tension measurements to the study of conformational transitions in aqueous solutions of poly-L-lysine

The change in surface tension of solutions of poly-L -lysine in water has been studied as a function of temperature at various pH values. The changes at various temperatures have been correlated with changes in the circular dichroic spectra reflecting conformational change. In addition to the major transition at 50°C attributed to the conversion of the α-helical → β conformation, two other transitions have been observed at 30°C and 80°C. A minimum in the surface tension value was observed at pH 10, near the pK value for poly-L -lysine. It was concluded that at this pH the concentration of hydrophobic groups at the surface was a maximum.     

Raman spectra of poly-L-lysines

The Raman spectra of poly-L -lysine hydrochloride and poly-?-carbobenzoxy-L -lysine in the solid state have been obtained and are consistent with the presence of an α-helical structure. The Raman spectrum of poly-L -lysine in aqueous solution suggests the presence of random coil structures.     

Effect of side chains on the conformational energy and rotational strength of the n-pi transition for some alpha-helical poly-alpha-amino acids

Calculations of the dependence of the conformational energy and the rotational strength of the amide n–π* electronic transition (in a series of α-helical polyhel-α- amino acids with different side chains) on conformation have been carried out. The conformational energies were computed by procedures developed in this laboratory; the computation of rotational strengths was carried out by the method of Schellman and Oriel, with a slight modification. Polyamino acids with both nonpolar and polar side chains were considered; in the latter case, it was assumed that the only influence of the polar side chain was on the backbone conformation and on the electrostatic field which perturbs the amide chromophore of the backbone. Only conformations in the range of backbone dihedral angles of the right- and left-handed a-helices were considered, and the assumption of regularity (i.e., uniformity of dihedral angles in every residue) was made. The rotational strength per residue was found to vary markedly with chain length (in oligomers of up to 40 residues long); both the conformational energy per residue and the rotational strength per residue were found to vary significantly with the backbone conformation, which in turn depends on the nature of the side chain. The geometry of the hydrogen bond in the α-helical backbone is the most important factor which influences the dependence of the rotational strength on conformation. The implications of these results, for the interpretation of experimental circular dichroism and optical rotatory dispersion data, are discussed.     

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.     

Influence of isopropanol-water solvent mixtures on the conformation of poly-L-lysine

The helix–coil transition of poly-L -lysine (PLL) in water–isopropanol solvent mixtures has been investigated at room temperature by circular dichroism measurements. Within the range of 70%–80% isopropanol concentration (by volume), the polymer undergoes a sharp transition, characterized by the formation of a fully charged α-helical structure. On the basis of some experimental evidence the role of the organic component in solution appears more complicated than that of strengthening the intramolecular hydrogen bonds in the polymer. By analogy with the distribution of the components of alcohol–water mixtures in simple ionic systems, it is thought that only an high co-solvent concentration brings about an extensive and possible cooperative depletion of the clusters of firmly-bound water molecules in the domain of the polylelectrolyte, favoring the transition to the α-helical structure. On the other hand, CD spectral patterns show that the addition of NaCl in the alcohol-rich–water mixtures of charged poly-L -lysine gives rise to a transition from the α-helical to a β-structures conversion obeys a first-order rate law at all times, with a rate constant dependent on solvent composition and ionic strength. In these conditions, the rate of the process is close to that found for the thermally induced α–β transition. Higher polymer concentration and/or ionic strength cause a phase separation of β-PLL, suggesting that in this case interchain reactions (where hydrogen bonding should play the major role) predominate. Titration experiments on charged α-helical poly-L -lysine in 85% or 90% isopropanol mixtures confirm the occurrence of a conformational transition, which takes place within a degree of dissociation α of 0.2–0.75. The transition is accompanied by a visible turbidity, which increases as the titration proceeds. Implications of the solvent distribution around the macroion on the observed conformational phenomena are also discussed.     

Conformations of poly-L-valine in solution

In order to test theoretical predictions that poly-L -valine can exist in an α-helical conformation, water-soluble block copolymers of L -valine and D , L -lysine were prepared. By carrying out the synthesis on a resin support (with the use of N-carboxyanhydrides) contamination of the individual blocks by any unreacted monomer from the previous block was avoided. A single glycine residue was incorporated at the C-terminus of the chain for use in amino acid analyses. Using optical rotatory dispersion and circular dichroism criteria, about 50% of the short valine block of (D , L -lysine HCl)₁₈-(L -valine)₁₅-(D , L -lysine-HCl)1₆-glycine was found to be in the right-handed α-helical conformation in 98% aqueous methanol, in water, the polymer appears to be a dimer, with the valine block being involved in the formation of an intermolecular β-structure.     

Raman spectra of D and L amino acid copolymers. Poly-DL-alanine, poly-DL-leucine, and poly-DL-lysine.

The Raman spectrum of poly-DL -alanine (PDLA) in the solid state is interpreted in terms of the disordered chain conformation, in analogy with the spectrum of mechanically deformed poly-L -alanine. The polymer is largely disordered with only a small α-helical content in the solid state. When PDLA is dissolved in water, the spectra suggest that short α-helical segments are formed upon dissolution. These helical regions might be stabilized by hydrophobic bonds between side-chain methyl groups. Addition of methanol to the aqueous PDLA solutions results in a Raman spectrum resembling that of solid PDLA. This result suggests that the methanol disrupts the helical regions by breaking the hydrophobic bonds. The Raman spectra of poly-DL -leucine (PDLL) and poly-L -leucine (PLL) are compared and only slight differences are observed in the amide I and III regions, indicating that PDLL does not have an appreciable disordered chain content. Significant differences are observed in the skeletal regions. The 931-cm^?1 lines in the PLL and PDLL spectra are assigned to residues in α-helical segments of the preferred screw sense, i.e., L -residues in right-handed segments and D -residues in left-handed segments (in PDLL). On the other hand, the 890-cm^?1 line in the spectrum of PDLL is assigned to residues not in the preferred helical sence, i.e., L -residues in left-handed segments and D -residues in right-handed ones. The Raman spectra of poly-DL -lysine and poly-L -lysine in salt-free water at pH 7.0 are compared. The Raman spectra of the two polymers are very similar. However, this does not negate the hypothesis of local order in poly-L -lysine because the distribution of the residues in poly-DL -lysine probably tends towards blocks, and the individual blocks may take up the 3₁ helix.     

Spectroscopic studies of random chain and -helical polypeptides in hexafluoroisopropanol

The infrared, ultraviolet, circular dichroism, and optical rotatory dispersion spectra of five synthetic polypeptides dissolved in hexafluoroisopropanol are reported. This solvent is useful because it dissolves most proteins and non-ionic polypeptides and also is transparent in spectral regions critical for polypeptide conformational diagnoses. Poly-γ-morpholinylethyl-L -glutamamide has random chain type spectra in this solvent, whereas the spectra of poly-γ-methyl-L -glutamate, poly-L -methionine, poly-ε, N -Carbo-benzoxy-L -lysine, and poly-L -homoserine indicate that these four polypeptides are α-helical. Small but significant variability between the different α-helical polypeptides is seen in their circular dichroism spectra and optical rotatory dispersions. An argument is presented that these differences may be due to slight geometry differences between different α-helices.     

Proton magnetic resonance studies on conformation and association of oligo-γ-benzyl-L-glutamates in solution

The proton magnetic resonance spectra of o-nitrophenylthio-tetra- and hexa-γ-benzyl-L -glutamate ethylamides have been measured at different concentrations in CDCl₃ and CD₂₂C1. The NH and α-CH resonances of the tetrapeptide show downfield shifts with increasing concentration, accompanying disappearance of their fine structure and line broadening. The apparent feature of chemical shifts against concentration is sigmoidal, and it can be interpreted by assuming the presence of a step or more of association–dissociation equilibria of tetrapeptide. With increasing concentration, small aggregates are formed by intermolecular hydrogen bonding, the size of which is not sufficiently large to exhibit critical micelle concentrations. In contrast to the tetrapeptide, the hexapeptide has constant chemical shifts of the NH and α-CH resonances, independent of concentration, which implies that only the unassociated molecules show observable sharp resonances. In the hexapeptide, the phenyl CH and benzyl CH₂ groups of the side chains exhibit new resonances above certain critical concentrations, indicating the restriction of rotational freedom of the side chains in the aggregated states.     

A comparative study on bovine alpha-lactalbumin and lysozyme by nanosecond fluorometry.

Analysis of the time decay of fluorescence anisotropy of 1-dimethylaminoaphthalene-5-sulfonyl (DNS) and fluorescamine derivatives of bovine alpha-lactalbumin and lysozyme reveals that no significant differences in mean rotational relaxation times are present. While fluorescamine molecules appear to orient randomly on these proteins, DNS is bound with a preferential orientation. Other fluorescence characteristics of the labels are also cited.     

Single crystals of poly-L-lysine

Crystals of poly-L -lysine have been grown from aqueous solution in the presence of divalent anions. The most stable of these incorporate the HPO ion and are precipitated by the addition of sodium monohydrogen phosphate to solutions of poly-L -lysine HBr. Precipitation at or slightly above room temperature gives rise to single crystals of α-poly-L -lysine HPO₄ in the form of hexagonal lamellae about 150 Å thick. The axes of the helical polypeptide molecules are oriented normal to the planes of the lamellae, and since molecular length is about 1100 Å in the α-helical conformation, these helices must be folded. The a parameter of the hexagonal unit cell is 19.55 Å for crystals immersed in mother liquor, and the lysine side chains are almost fully extended. Precipitation brought about by heating the same solutions to about 75°C produces micro-crystals of β-poly-L -lysine HPO₄. A mode of packing of the anions in these crystals is proposed tentatively on the basis of an intersheet spacing determined from x-ray powder diffraction patterns. In general, α crystals are transformed to β structures on drying; conditions under which the transition can either be forestalled or reversed are discussed.     

Recognition and Binding of a Helix-Loop-Helix Peptide to Carbonic Anhydrase Occurs via Partly Folded Intermediate Structures

We have studied the association of a helix-loop-helix peptide scaffold carrying a benzenesulfonamide ligand to carbonic anhydrase using steady-state and time-resolved fluorescence spectroscopy. The helix-loop-helix peptide, developed for biosensing applications, is labeled with the fluorescent probe dansyl, which serves as a polarity-sensitive reporter of the binding event. Using maximum entropy analysis of the fluorescence lifetime of dansyl at 1:1 stoichiometry reveals three characteristic fluorescence lifetime groups, interpreted as differently interacting peptide/protein structures. We characterize these peptide/protein complexes as mostly bound but unfolded, bound and partly folded, and strongly bound and folded. Furthermore, analysis of the fluorescence anisotropy decay resulted in three different dansyl rotational correlation times, namely 0.18, 1.2, and 23 ns. Using the amplitudes of these times, we can correlate the lifetime groups with the corresponding fluorescence anisotropy component. The 23-ns rotational correlation time, which appears with the same amplitude as a 17-ns fluorescence lifetime, shows that the dansyl fluorophore follows the rotational diffusion of carbonic anhydrase when it is a part of the folded peptide/protein complex. A partly folded and partly hydrated interfacial structure is manifested in an 8-ns dansyl fluorescence lifetime and a 1.2-ns rotational correlation time. This structure, we believe, is similar to a molten-globule-like interfacial structure, which allows segmental movement and has a higher degree of solvent exposure of dansyl. Indirect excitation of dansyl on the helix-loop-helix peptide through Förster energy transfer from one or several tryptophans in the carbonic anhydrase shows that the helix-loop-helix scaffold binds to a tryptophan-rich domain of the carbonic anhydrase. We conclude that binding of the peptide to carbonic anhydrase involves a transition from a disordered to an ordered structure of the helix-loop-helix scaffold.     

Effect of quinone on the fluorescence decay dynamics of endogenous flavin bound to bacterial luciferase

The interaction of quinone with luciferase from Photobacterium leiognathi was studied based on the fluorescence decay measurements of the endogenous flavin bound to the enzyme. Homologous 1,4-quinones, 1,4-benzoquinone, methyl-1,4-benzoquinone, 2-methyl-5-isopropyl-1,4-benzoquine and 1,4-naphthoquinone, were investigated. In the absence of quinone, the fluorescence intensity and anisotropy decays of the endogenous flavin exhibited two intensity decay lifetimes (~ 1 and 5 ns) and two anisotropy decay lifetimes (~ 0.2 and 20 ns), suggesting a heterogeneous quenching and a rotational mobility microenvironment of the active site of the luciferase, respectively. In the presence of quinone, the intensity decay heterogeneity was largely maintained, whereas the fraction of the short anisotropy decay component and the averaged rotational rate of FMN increased with the increasing hydrophobicity of the quinone. We hypothesize that the hydrophobicity of the quinone plays a role in the non-specific inhibition mechanism of xenobiotic molecules in the bacterial bioluminescence system via altering the rotational mobility of the endogenous flavin in the luciferase.     

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.     

Segmental flexibility of the C1q subcomponent of human complement and its possible role in the immune response

Fluorescence polarization techniques were used to study the rotational dynamics of the C1q subcomponent of human complement. C1q was covalently labeled with dansyl (DNS) chloride. Digestion of either C1q-DNS4.0 or C1q-DNS1.8 conjugates with pepsin showed that about 75% of the DNS probes were attached to the C1q globular heads and that the remainder were on the collagen-like stalk (peptic fragment). C1q-DNS conjugates readily agglutinated IgG-coated latex beads and combined with C1r2C1s2 to form hemolytically active 16 S C1-DNS. Both C1q-DNS and C1-DNS samples displayed steady-state rotational correlation time and fluorescence lifetime transitions near 48 degrees C. Hydrodynamic studies showed that C1q formed soluble aggregates near the transition temperature. In contrast, stalk samples with a DNS probe apparently attached to the large central fibril showed no thermal transitions or aggregation even when heated above 50 degrees C. Nanosecond fluorescence depolarization measurements detected restricted flexible motions of the C1q heads with an associated rotational correlation time, phi s, of about 25 ns. The C1q anisotropy decay was dominated, however, by a long component, phi L, of perhaps 1000 ns. Except for probe wiggle, the stalk-DNS anisotropy profile was essentially flat. The rapid rotations associated with phi s could represent restricted twisting motions of the arm-head segments or wobbling motions of the heads themselves. Such motions may facilitate binding of the C1q heads to immune complexes. Straightforward diffusion calculations indicated that phi L could represent either global tumbling of the entire C1q molecule or wagging motions of the individual arm-head segments, as suggested by electron micrographs. Upon binding of the C1q heads to an activator, some of the C1q segments may be held in a slightly more open or more closed conformation, which in turn may trigger activation of the C1 proenzymes. In conclusion, we suggest a plausible triggering mechanism for C1 activation that is compatible with the flexible properties of its subcomponents.     

Kinetic studies on the helix-coil transition of fluorescent labeled poly(-L-lysine) by the temperature-jump technique

Fluorescent dansyl labels were covalently attached to poly (L-lysine) (poly(Lys)) with a degree of polymerization of 300 to 600. The degree of labeling was 0.01 to 0.085 (mol label to mol amino acid residues). From the decay of the anisotropy of fluorescence it was concluded that the labels were highly mobile both in the coiled and helical state. A decrease of fluorescence intensity accompanied the helix-coil transition. Identical pH induced transition curves were measured by circular dichroism and fluorescence. The midpoint of the transition was at pH 10.2. The kinetics of the transition were studied by temperature-jump relaxation using fluorescence detection. A single relaxation phase was observed. The relaxation time tau exhibited a distorted bell shaped dependence on the degree of helicity f with a maximum value tau(max) = 15 micros at f = 0.3 and 20 degrees C. It was independent of polymer concentration and of the degree of labeling. A rate constant of helix propagation kF = 10(7) s(-1) was calculated from tau(max) and published values of the nucleation parameter sigma. The activation energy was 16 kJ mol . The observed rate constant is comparable to that of poly(L-glutamic acid) but two orders of magnitude smaller than that found for polyamino acids with nonionizable side chains.