An X-ray diffraction study of poly-L-arginine hydrochloride

An x-ray study has been made of polyarginine hydrochloride to investigate whether, like polylysine hydrochloride, it can undergo conformational changes merely from variations in the degree of hydration. X-ray powder and fiber photographs of specimens containing up to about five molecules of water per arginine residue show features characteristic of α-helical structures including a 5.4-Å layer line and a meridional 1.5-Å reflection. Increasing the water content from ¹/₂ to 6¹/₂ molecules per residue causes the a axis of the hexagonal unit cell to increase from 14.4 Å to 15.8 Å, with no appreciable change in the 27.0 Å c axis. Removal of the last half molecule of water results in a very diffuse α pattern, but on rehydration the sharp pattern reappears. Specimens containing five to twenty water molecules per residue show quite a different pattern, the spacing of which do not vary appreciably with hydration. This pattern includes a meridional 3.4-Å reflection, a feature commonly shown by β structures, and indeed all the reflections can be satisfactorily indexed in terms of a monoclinic unit cell with a = 9.26 Å, b = 22.05 Å, c = 6.76 Å, and γ = 108.9°. These dimensions are shown by models to be compatible with a β pleated-sheet structure.     

An X-ray diffraction study of poly(L-lysine hydrobromide)

A structural study of the synthetic polypeptide poly(L -lysine hydrobromide) has been made by X-ray fiber techniques. The investigation was undertaken to determine whelther this polymer undergoes conformational transitions as a function of hydration in a manner similar to other chemically related basic polypeptides. Specifically, a comparison with the previously reported structures of the hydrochloride form of poly(L -lysine) was sought. Homogeneous powder mixtures with various amounts of water and oriented fibers of poly(L -lysine hydrobromide) at different relative humidities were X-ray photographed. Reversible transitions amorphous state ? β-pleated sheet ? α-helix ? isotropic solution as a function of increasing/decreasing degrees of hydration were found. The β-pleated-sheet conformation was observed between 33% and 76% relative humidities (containing about one and three molecules of water per residue, respectively). Each pleated sheet was formed by “antiparallel” chains, and the sheets were piled up along the b-axis. The spacings of this conformation did not vary appreciably with hydration. The observed reflections at 52% relative humidity (1.4 molecules of water per residue) could be indexed satisfactorily in terms of an orthorhombic unit cell, of space group P2₁22₁, with a = 9.52 Å, b = 16.44 Å, and c = 6.80 Å. These dimensions were shown by models to be compatible with the proposed structure. The α-helix conformation was present in specimens photographed at 76% relative humidity and up, and containing between three and fifteen molecules of water per residue. The helices were packed parallel to each other in a hexagonal array but randomly along or about their lengths. Increasing the hydration from five to fifteen molecules of water per residue causes the a-axis to increase from 16.9 to 20.8 Å. Twenty molecules of water per residue produced an isotropic solution. Despite some structural differences between the hydrobromide and hydrochloride forms it is concluded that the role played by the anions is mainly related to determining the water content levels at which conformational changes occur. Therefore, the anions do not significantly influence the prevailing conformation in this particular system, but might affect the packing arrangement of the polypeptide chains.     

An X-ray diffraction study of poly-L-homoarginine hydrochloride.

An X-ray study of the synthetic polypeptide poly(L -homoarginine hydrochloride) has been made to investigate whether, like the chemically related polypeptides poly(L -lysine hydrochloride), poly(L -arginine hydrochloride), and poly(L -ornithine hydrobromide), it can undergo conformational transitions merely from variations in its degree of hydration. X-ray photographs of powder and oriented specimens containing one to 15 molecules of water per L -homoarginine hydrochloride residue showed that this polymer forms only a β-pleated-sheet structure. The pleated sheets, formed by antiparallel polypeptide chains hydrogen-bonded to each other, are piled up along the b axis in an alternating sequence (“sandwich structure”). This structure did not appreciably change with variations of the degree of hydration, and the observed reflections at 56% relative humidity (1.8 molecules of water per residue) could be indexed satisfactorily in terms of a monoclinic unit cell, of space group P2₁, with a = 9.34 Å, b = 40.07 Å, c = 6.94 Å, and γ = 106°. These dimensions are shown by models to be compatible with the proposed structure, and the calculated density of 1.27 g/cm³ agrees well with the experimental value of 1.29 g/cm³. Removal of the last molecule of water results in a very diffuse pattern, while specimens containing 20 molecules of water per residue show only reflections due to water.     

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.     

Calorimetric measurement of enthalpy change in the isothermal helix--coil transition of poly-L-lysine in aqueous solution

The heat ΔH° for converting an uncharged lysine residue from a coil to an α-helical state in poly-L -lysine in 0.1N KCl has been determined calorimetrically to be ?1200 cal/mole at both 15°C and 25°C. Essentially the same value has been obtained for the conversion of an uncharged residue from a coil to a β-pleated sheet state. Titration data provided information about the state of charge of the polymer in the calorimetric experiments, and optical rotatory dispersion data about its conformation. In order to compute ΔH°, the observed Calorimetric heat was corrected for the heat of breaking the sample cell, the heal of dilution of HCl, the heat of neutralization of OH^? ion, and the heat of ionization of the ε-amino group in the random coil. The latter was obtained from similar Calorimetric measurements on poly-D ,L -lysine, which was shown to be a good model for the random coil form of poly-L -lysine. The measured transition heat was ～0.7 cal., which is only 7% of the total heat liberated when a 40 ml solution of 0.25% w/v poly-L -lysine is brought, from pH 11 to pH 7; nevertheless it could be determined with a precision of ±8%. The conformation of poly-L -lysine at pH 11 appears to be completely helical at 15°C, but a mixture of 90% α-helix, 5% β form, and 5% coil at 25°C. Since ΔH° ～ 0 for the α ? β conversion, the polymer behaves like one of 95% α-helix and 5% coil in the calorimeter at 25°C. At neutral pH, poly-L -lysine is an extended coil, like poly-D ,L -lysine.     

Volume and sound velocity changes accompanying the -helix to -form and coil to -helix transitions in aqueous solution

The volume increment per amino acid residue for the α-helix to β-form transition of uncharged poly-L -lysine in aqueous solution was 3.8 ml in water and 4.3 ml in 0.2M and 1M NaBr solutions at 26°C, respectively. The sound velocity of the polymer solution was greater with the β-helix than with the β-form, but the difference was less in dilute salt solutions and disappeared in 1 or 2M NaBr solution. Thus, the β poly-L -lysine solution was slightly more compressible than the α-polymer solution, but this difference was diminished with increasing salt concentration. Both the volume change and the change in adiabatic compressibility of the polymer solution suggest that hydrophobic interactions among the lysyl groups in the β-form reduce the amount of “icebergs” surrounding the polymer molecules as compared with the amount originally present with the α-helix. The coil-to-helix transition of poly-L -glutamic acid in aqueous solution was also accompanied by a decrease in sound velocity. This can be attributed to the reduction of the water of hydration which is less compressible than free water.     

Experimental conformational study of two peptides containing α-aminoisobutyric acid. Crystal structure of N-acetyl-α-aminoisobutyric acid methylamide

Some theoretical studies have predicted that the conformational freedom of the α-aminoisobutyric acid (H-Aib-OH) residue is restricted to the α-helical region of the Ramachandran map. In order to obtain conformational experimental data, two model peptide derivatives, MeCO-Aib-NHMe 1 and Bu^tCO-LPro-Aib-NHMe 2 , have been investigated. The Aib dipeptide 1 crystallizes in the monoclinic system (a = 12.71 Å, b = 10.19 Å, c = 7.29 Å, β = 110.02°, Cc space group) and its crystal structure was elucidated by x-ray diffraction analysis. The azimuthal angles depicting the molecular conformation (? = ?55.5°, ψ = ?39.3°) fall in the α-helical region of the Ramachandran map and molecules are hydrogen-bonded in a three-dimensional network. In CCl₄ solution, ir spectroscopy provides evidence for the occurrence of the so-called ₅ and C₇ conformers stabilized by the intramolecular i → i and i + 2 → i hydrogen bonds, respectively. The tripeptide 2 was studied in various solvents [CCl₄, CD₂Cl₂, CDCl₃, (CD₃)₂SO, and D₂O] by ir and pmr spectroscopies. It was shown to accommodate predominantly the βII folded state stabilized by the i + 3 → i hydrogen bond. All these experimental findings indicate that the Aib residue displays the same conformational behavior as the other natural chiral amino acid residues.     

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.     

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.     

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.     

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     

Nmr studies of mixtures of poly-L-lysine hydrobromide with water

¹H, ²H, ¹³C, and ⁸¹Br nmr measurements of mixtures of poly-L -lysine hydrobromide with water have been carried out over a range of temperatures and water contents. When n (number of molecules of water per residue) ～13 at room temperature, a transition occurs from a gel to a liquid phase. The liquid phase contains polymer molecules that are flexible, but contain more intramolecular structure than the same molecules in trifluoracetic acid solution. The gel phase contains junction zones of hexagonally packed α-helices, linked by flexible regions of polypeptide chain. The α-helical residues impart to their associated water molecules a slight anisotropy of motion, which is dectable by ²H nmr. These residues bind up to about seven molecules of water each; the other six required to complete the gel–liquid transition space out the polymer molecules, allowing increased segmental motion of the residues in the flexible regions. This increased motion reduces the energy of the flexible regions and thus increases the proportion of residues in them (increasing the temperature has the same effect); the transition occurs when insufficient residues remain in the α-helical junction zones.     

Side-chain conformation in poly(γ-phenethyl-L-glutamate)

X-ray diffraction and energy-minimization results are reported for poly(γ-phenethyl-L -glutamate). Orthorhombic unit-cell parameters of drawn fibers are a = 15.4 Å, b = 26.6 Å, c = 54.4 Å. Atomic coordinates are derived for an α-helix peptide conformation that corresponds to a calculated side-chain internal energy minimum. The side-chain conformation correlates well with the electron density projection; the side chains wrap around the α-helical main chain with the phenethyl ester group directed toward the N-terminus. The para-axis of the benzene ring is inclined at an angle nearly nearly normal to the helix axis. The x-ray structure factors calculated for this model, when compared to the 10 observed structure factors, yield a crystallographic reliability index of R = 0.23.     

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.     

Interaction between chondroitin-6-sulfate and poly-L-arginine in aqueous solution

The interactions between chondroitin-6-sulfate and poly-L -arginine in aqueous salt solution have been investigated by circular dichroism techniques. In the presence of chondroitin-6-sulfate, at neutral pH, poly-L -arginine adopts the α-helical conformation rather than “charged coil” form observed in the absence of mucopolysaccharide. This interaction is at a maximum when the ratio of arginine to disaccharide residues is 2:1. Elevation of the temperature leads to a sharp melting transition at 76.0 ± 1.0°C. This behavior is in marked contrast to that for poly-L -lysine-chondroitin-6-sulfate interactions, which are at a maximum at a 1:1 residue ratio and have a melting transition at 47.0 ± 1.0°C. These results indicate a stronger interaction for poly-L -arginine than for poly-L -lysine. The positive arginine side chains appear to interact with both the negative sulfate and carboxyl residues, while those of the lysines are involved only with the sulfates. Poly-L -ornithine at neutral pH shows no conformation directing interaction with chondroitin-6-sulfate, although a small proportion of α-helix is formed on dilution of the mixture with methanol. The extent of the interaction of cationic polypeptides with chondroitin-6-sulfate increases in the order poly-L -ornithine, poly-L -lysine, poly-L -arginine, i.e., in the order of increasing side-chain length.     

Crystallization and preliminary crystallographic study of the pentamerizing domain from cartilage oligomeric matrix protein: A five-stranded α-helical bundle

Cartilage oligomeric matrix protein (COMP) is a pentameric glycoprotein of the thrombospondin family found in cartilage and tendon. Self-association of COMP is achieved through the formation of a five-stranded α-helical bundle that involves 64 N-terminal residues (from 20 to 83). The complex is further stabilized by the interchain disulfide bonds between cysteines 68 and 71. We have prepared, by expression in Escherichia coli, several peptides of different lengths from the N-terminal region of COMP and studied their amenability to crystallization. Crystals of the best quality were obtained with a peptide spanning COMP residues 28–72. This peptide forms disulfide linked pentamers with 87% of α-helical structure. Crystals were grown by the hanging drop vapor diffusion method, using polyethylene glycol 1500 as a precipitant. The crystals belong to space group P2₁ with unit cell dimensions a = 38.47 Å, b = 49.47 Å, c = 54.98 Å, β = 103.84° and contain one pentamer per asymmetric unit. They diffract strongly to at least 1.8 Å resolution.     

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.     

Chain length dependent transition of 310- to α-helix of Boc-(Ala-Aib)n-OMe

An apolar synthetic octapeptide, Boc-(Ala-Aib)₄-OMe, was crystallized in the triclinic space group P1 with cell dimensions a = 11.558 Å, b = 11.643 Å, c = 9.650 Å, α = 120.220°, β = 107.000°, γ = 90.430°, V = 1055.889 ų, Z = 1, C₃₄H₆₀O₁₁N₈·H₂O. The calculated crystal density was 1.217 g/cm³ and the absorption coefficient ? was 6.1. All the intrahelical hydrogen bonds are of the 3₁₀ type, but the torsion angles, ? and ψ, of Ala(5) and Ala(7) deviate from the standard values. The distortion of the 3₁₀-helix at the C-terminal half is due to accommodation of the bulky Boc group of an adjacent peptide in the nacking. A water molecule is held between the N-terminal of one peptide and the C-terminal of the other. The oxygen atom of water forms hydrogen bonds with N (1) -H and N (2) -H, which are not involved in the intrahelical hydrogen bonds. The hydrogen atoms of water also formed hydrogen bonds with carbonyl oxygens of the adjacent peptide molecule. On the other hand, ¹H-nmr analysis revealed that the octapeptide took an α-helical structure in a CD₃CN solution. The longer peptides, Boc-(Ala-Aib)₆-OMe and Boc-(Ala-Aib)₈-OMe, were also shown to take an α-helical structure in a CD₃CN solution. An α-helical conformation of the hexadecapeptide in the solid state was suggested by x-ray analysis of the crystalline structure. Thus, the critical length for transition from the 3₁₀- to α-helix of Boc-(Ala-Aib)_n-OMe is 8. © 1993 John Wiley & Sons, Inc.     

Small-angle x-ray scattering by poly-L-alanine solutions

The radius of gyration and “persistence length” of poly-L -alanine, calculated from small-angle x-ray scattering data, have values of 56 Å and 44 Å, respectively, in dichloroacetic acid, and 78 Å and ～30 Å in a 1:1 v/v mixture of trifluoroacetic acid and trifluoroethanol. This can be interpreted to mean that poly-L -alanine exists in a relatively rigid, predominantly α-helical conformation in dichloroacetic acid and in an extended, more flexible form in the mixed solvent system.