Light-scattering and potentiometric-titration studies of poly-L-tyrosine in aqueous solution

Aqueous solutions of poly-L -tyrosine were studied by potentiometric titrations, light-scattering measurements, and infrared spectroscopy in order to characterize the conformational changes the macromolecules exhibit when the hydrogen-ion concentration of the solutions is varied. It was found that when the pH of the system at 25°C is lowered from a value of about 13 the poly-L -tyrosine molecules undergo a random-coil to β-structure conformation change at pH 11.5. It appears, that under the experimental conditions used, the formation of the β structure is an intramolecular process which involves the folding of the polymer backbone into several hairpins of antiparallel β structure. On further lowering of the pH of the solutions aggregation (pH 11.35) and subsequently precipitation (pH 11.2) takes place. Since the apparent pK of the polymer does not show a drastic change during the random-coil to β-structure conformation change, it was concluded, that the therinodynamic driving force for this conformation change is mainly due to the electrostatic effect of the partially charged side chains of the poly-L -tyrosine molecules.     

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.     

Calculation of the molecular parameters of the alpha-helix-coil and beta-structure-coil transitions.

Monte-Carlo calculations of geometric and thermodynamic characteristics of the α-helix and the β-structure of polypeptides have been carried out. To describe a hydrogen bond both the Lippincott–Schroeder and Morse potentials were used. The internal rotation angles φ and ψ in the α-helix have been shown to fluctuate in the range of ±7°. The distribution functions on angles φ and ψ and on hydrogen bond lengths and angles in the α-helix have been computed and compared with those in myoglobin and lysozyme. Thermodynamic characteristics of the α-helix calculated in different approximations with the two forms of the hydrogen bond potentials have also been compared. The data obtained are close to the experimental values for polypeptides in neutral solution. Some geometric and thermodynamic characteristics of the regular parallel and antiparallel and irregular antiparallel β-structure have been found. In the β-structure the internal rotation angles vary within the interval ±15–20°. An increase in the cross and longitudinal dimensions of the β-structure only slightly influence both the geometric and thermodynamic characteristics.     

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.     

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.     

COMPARISON OF THE BINDING’ OF β-ALANINE AND y-AMINOBUTYRIC ACID IN SYNAPTOSOMAL-MITOCHONDRIAL FRACTIONS OF RAT BRAIN1

Abstract— Na⁺-dependent ‘binding’ of β-alanine and GABA was examined with synaptosomal-mitochondrial fractions of rat brain incubated for 10 min at 0°C. GABA was bound to a much greater extent than β-alanine to particles of cerebral cortex, whole cerebellum and brain stem. For cerebral cortex, the binding capacity (B_max) for GABA was about 18 limes greater than that for β-alanine. and the affinity of the particles for GABA was about 2′ times greater than for β-alanine. The order of potency of GABA binding to brain regions was cerebral cortex > cerebellum > brain stem, whereas that for β-alanine was the reverse. If the binding of β-alanine is taken to indicate the glial component of the Na⁺-dependent binding process for GABA, then most of the GABA was bound to neuronal elements under the conditions employed.     

Neutron-scattering spectroscopy of the alpha- and beta- forms of poly-L-alanine. Motion of the methyl side chain.

Detailed inelastic, incoherent neutron-scattering (INS) spectra are presented for poly-L -alanine in both the α-helical and β-sheet form. Assignments are made from previous normal coordinate calculations. Of particular interest is the methyl torsion at 230 cm^?1, which is the strongest peak in the spectrum and is independent of backbone conformation. The height of the potential barrier for methyl group rotation is calculated to be 14 kJ mol^?1.     

Conformational properties of Pro-Pro sequences. I. Crystal structures of two dipeptides with L-Pro-L-Pro and L-Pro-D-Pro sequences

The crystal structures of Bu^tCO-L -Pro-L -Pro-NHMe, H₂O (1: monoclinic; P2₁; a = 6.662, b = 11.067, c = 12.205 Å; β = 96.28°) and Bu^tCO-L -Pro-D -Pro-NHMe (2: monoclinic; P2₁; a = 10.770, b = 15.039, c = 11.325 Å; β = 110.00°) have been solved by x-ray diffraction. Structure 1 accommodates an open disposition with intermolecular interactions involving the water molecule, while 2 is βII-folded by an intramolecular i + 3 → i hydrogen bond. In both derivatives, small thermal parameters are indicative of fairly fixed conformations for the proline rings. Comparison between conformations of either isolated or adjacent L -Pro residues in the crystal structures of unstrained oligopeptides shows that the conformational properties of L -Pro-L -Pro sequences are probably a simple combination of those found for isolated L -Pro residues.     

Crystal and molecular structure of cyclohepta-amylose dodecahydrate

β-Cyclodextrin (cyclohepta-amylose, β-CD) is a torus-shaped, cyclic heptasaccharide consisting of (1→4)-linked α-d-glucopyranosyl residues. It is able to form inclusion complexes with small molecules in aqueous solution because of its annular aperture (width, 6.2 Å). β-Cyclodextrin dodecahydrate, the “empty” β-CD, crystallises from water in space group P2₁, with cell constants a = 21.29(2), b = 10.33(1), c = 15.10(2) Å, and β = 112.3(5)°. A total of 5189 X-ray counter-data were collected on a four-circle diffractometer. The crystal structure was solved on the basis of the highly isomorphous β-CD · 2HI · 8H₂O adduct, and the atomic parameters were refined by the full matrix, least-squares method to R = 7.3% for all data. The crystal structure belongs to the cage type. The β-CD macrocycle exists in an open, circular conformation stabilised by intramolecular hydrogen-bonds between HO-2 and HO-3 of adjacent glucosyl residues; four of the seven HO-6 groups are in the favoured (?)gauche orientation with respect to O-5, two are in the (+)gauche orientation, and one is disordered over these two orientations. The 6.5 water molecules within the cavity are distributed over 8 sites and display extensive thermal motion which is probably correlated with statistical disorder.     

Optical properties of polypeptides in the β-conformation

The rotational strengths and oscillator strengths of the nπ* band and ππ* exciton bands have been calculated for antiparallel and parallel β-structures of varying length and width. The results are compared with experiment and with previous theoretical treatments of β-structures. The generally good agreement of calculations on the antiparallel β-structure with experimental results on poly-L -lysine and poly-L -serine indicates that these systems are indeed in the antiparallel conformation. It is found that the exciton component strongest in absorption shifts to longer wavelengths as the width of an antiparallel structure increases, and it is suggested that the position of the ππ* absorption band may be a useful criterion of sheet width. The results also reconcile the linear dichroism measurements of Rosenheck and Sommer on poly-L -lysine films with an anti-parallel structure. Calculations on parallel β-structures indicate that the CD spectra of this form will be rather similar to that of the antiparallel form. However, the major absorption band in the antiparallel form is associated with a small positive CD band, while in the parallel form it coincides with a large negative CD band. Finally, it is pointed out that the large positive CD bands predicted for single-stranded parallel and antiparallel β-structures at about 200 mμ render unlikely the suggestion that random-coil polypeptides contain a substantial fraction of extended chain.     

Thermal and charge-induced coil to -helix transition of poly-L-glutamic acid and random L-glutamic acid-L-alanine copolymers

Thermal and charge induced random coil to α-helix transitions of poly-L -glutamic acid (PGA) were measured by optical rotatory dispersion in various solvents. The data of PGA in 0.1M Nacl were analyzed by the Zimm-Rice theory. Enthalpy and entropy changes for the coil-to-helix transition in the unionized state were obtained: ΔH° = ?1020 ± 100 cal/residue mole; ΔH° = ?3.0 ± 0.4 e.u./residue mole. The initiation parameter, σ, of the Zimm-Rice theory was given by a value of 5 ± 1 × 10^-3. Random copolymers of L -glutamic acid and L -alanine containing 10, 30, and 40 molar percents of alanyl residue were synthesized. Stabilities of α-helix of the copolymers were compared to that of PGA. In water and water-ethanol solutions, stabilities of the polymers were almost equal after the simple correction about the ionized charge density of the polymers. In 0.1 M NaCl solution these copolymers showed some deviations from the transition curve of PGA, which would suggest the hydrophobic contribution of the alanyl residues.     

Structural and conformational changes of β-lactoglobulin B: an infrared spectroscopic study of the effect of pH and temperature

Infrared spectra of 2.5 mM solutions of β-lactoglobulin B were recorded as a function of pH (from pH 2 to pH 13) and as a function of temperature (from −100°C to +90°C). An analysis of the pH- and temperature-induced changes in the secondary structures was performed based on changes in the conformation-sensitive amide I bands of β-lactoglobulin. Whereas the total of β-structure remains constant (56–59%) between pH22 and pH 10, the proportions of the various β-components do change. In particular, the dimerization of the monomeric protein, induced by raising the pH from 20 to 3, leads to an increase in the intensity of the 1636 cm⁻¹ band (associated with antiparallel β-sheet), at the expense of the 1626 cm⁻¹ band (associated with exposed β-strands). Both the thermal and alkaline denaturation of β-lactoglobulin occur in two distinct stages. Although the spectra (i.e., the structures) after complete thermal or alkaline denaturation are clearly different, the spectrum of the protein after the first stage of thermal denaturation (at about 60°C) is the same as that after the first stage of alkaline denaturation (at pH 11), suggesting a common denaturation intermediate, which probably represents a crossover point in a complex potential hypersurface.     

Synthesis,and crystal and molecular structure of the 310-helical α,β-dehydro pentapeptide Boc-Leu-Phe-Ala-ΔPhe-Leu-Ome

α,β-Dehydro amino acid residues are known to constrain the peptide backbone to the β-bend conformation. A pentapeptide containing only one α,β dehydrophenylalanine (ΔPhe) residue has been synthesized and crystallized, and its solid state conformation has been determined. The pentapeptide Boc-Leu-Phe-Ala-ΔPhe-Leu-OMe (C₃₉H₅₅N₅O₈, M_w = 721.9) was crystallized from aqueous methanol. Monoclinic space group was P2₁, a = 10.290(2)°, b = 17.149(2)°, c = 12.179(2) Å, β = 96.64(1)° with two molecules in the unit cell. The x-ray (Mo K_α, λ = 0.7107A) intensity data were collected using a CAD4 diffractometer. The crystal structure was determined by direct methods and refined using least-squares technique. R = 4.4% and R_w = 5.4% for 4403 reflections having |F₀| ≥ 3σ(|F₀|). All the peptide links are trans and the pentapeptide molecule assumes 3₁₀-helical conformation. The mean ?,ψ values, averaged over the first four residues, are ?64.4°, ?22.4° respectively. There are three 4 → 1 intramolecular hydrogen bonds, characteristic of 3₁₀,-helix. In the crystal, the peptide helices interact through two head-to-tail. N? H? O intermolecular hydrogen bonds. The peptide molecules related by 2₁, screw symmetry form a skewed assembly of helices. © 1995 John Wiley & Sons, Inc.     

1H- and 13C-NMR studies of N-acetyl-L-alanine methylester and N-acetyl-L-alanine methylamide. I. Self-association

The ¹H- and ¹³C-NMR spectra of N-acetyl-L -alanine methylester and N-acetyl-L -alanine methylamide were measured to examine the modes of self-association of these molecules in solution. The different dilution shifts between these molecules seem to correspond to the difference in the associated state for each molecule. Consequently, for the former molecule, a dimer model forming the intermolecular hydrogen bond through Ala NH hydrogen atom in one molecule to Ala C?O oxygen atom in another molecule was proposed. Another dimer model, which coincides with that proposed recently by Neel and coworkers, was proposed for the latter molecule. This second dimer model forms an intermolecular hydrogen bond through the NH of the N-methylamide group in one molecule to the acetyl C?O in another molecule.     

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.     

A potentiometric and CD investigation on the conformational properties of poly (L-p-aminophenylalanine) in aqueous solution

The conformational properties of poly(L -p-aminophenylalanine) have been investigated by potentiometric and circular dichroism (CD) techniques. It has been found that the polymer in the charge-free state can assume two ordered conformations, depending upon temperature conditions. At room temperature the polymer assumes the right-handed helical form by described Goodman and Peggion.¹ At temperatures higher than 40°C a new ordered conformation has been found, whose slow rate of formation and ir absorption properties are typical of the β-structure. The thermodynamic parameters relative to the coil-β transition, determined by potentiometric titration techniques, revealed that the thermodynamic stability of the β-structure is mainly due to enthalpic factors. The formation of this structure is unfavored on a kinetic basis.     

Structure of GlyGly peptide in the crystalline state as studied by X-ray diffraction and solid state 13C-NMR methods

A new type of crystal of glycylglycine (GlyGly) hydrate was crystallized from an aqueous solution, and the structure of the crystal has been determined by x-ray diffraction. The crystal is monoclinic, and the space group is C2/c, with the cell constants of a = 15.941(2) Å, b = 4.774(2) Å, c = 19.428(2) Å and β = 109.884(7)° at 296 K. There are eight GlyGly molecules and six water solvent in the cell. The GlyGly molecules are packed in a parallel β-sheet arrangement. The single crystal was obtained with a maximum size of 10 × 7 × 4 mm and is not stable under atmospheric conditions. The transparent crystal turned to turbid with the elapse of time. The isotropic ¹³C chemical shifts obtained from the ¹³C cross polarization magic angle spinning nmr experiments reveal that GlyGly hydrate was changed into GlyGly (form α) by dehydration. © 1998 John Wiley & Sons, Inc. Biopoly 45: 333–339, 1998     

X-ray diffraction studies on the structure of hydrated collagen

The temperature dependence of the humidity-sensitive spacing, d, related to the lateral packing of collagen molecules was measured for fully hydrated collagen. In the vicinity of 0°C, a sudden change in d was observed, which was reversible with temperature. In the diffraction profile, below 0°C, a set of diffraction peaks identified with the hexagonal crystalline form of ice was observed. With the reduction in water content, the intensity of the set of diffraction peaks decreased and was found to be zero at a water content of 0.38 g/g collagen. These results were considered to be caused by the frozen water in collagen fibril below 0°C. According to the water content dependence of d, it was considered that up to a certain water content water absorbed would be stowed in the intermolecular space of collagen and above that water content water molecules would aggregate to make pools, i. e., extrafibrillar spaces. The unfreezable bound water was considered to be located in the intermolecular space of collagen. Size of the extrafibrillar space, determined from the intensity analysis of a smallangle x-ray scattering pattern, corroborates the speculation that the water showed in the extrafibrillar space is freezable and free. The formation of the hexagonal crystalline form of ice in the extrafibrillar space was considered to cause the sudden change in d at 0°C.     

Phonon dispersion curves and normal coordinate analysis of -poly-L-alanine

The vibrational frequencies of α-helical poly-L -alanine and its N-deuterated analog have been assigned by normal coordinate analyses. The phonon dispersion curves and frequency distribution of α-poly-L -alanine have been calculated by using a model which includes hydrogen bonding. The frequency distribution was used to interpret the inelastic neutron scattering data and to calculate the heat capacity. The low-frequency chain modes involving accordian-like motions of the whole helix have been calculated and their dispersion investigated by means of a simplified model.     

Synthesis of β-alanine from l-aspartate using l-aspartate-α-decarboxylase from Corynebacterium glutamicum

β-Alanine is mainly produced by chemical methods in current industrial processes. Here, panD from Corynebacterium glutamicum encoding l-aspartate-α-decarboxylase (ADC) was cloned and expressed in Escherichia coli BL21(DE3). ADC _C.g catalyzes the α-decarboxylation of l-aspartate to β-alanine. The purified ADC _C.g was optimal at 55 °C and pH 6 with excellent stability at 16–37 °C and pH 4–7. A pH–stat directed, fed-batch feeding strategy was developed for enzymatic synthesis of β-alanine to keep the pH value within 6–7.2 and thus attenuate substrate inhibition. A maximum conversion of 97.2 % was obtained with an initial 5 g l-aspartate/l and another three feedings of 0.5 % (w/v) l-aspartate at 8 h intervals. The final β-alanine concentration was 12.85 g/l after 36 h. This is the first study concerning the enzymatic production of β-alanine by using ADC.