Small-angle X-ray scattering and rheological characterization of alginate gels. 3. Alginic acid gels

Alginic acid gels were studied by small-angle X-ray scattering and rheology to elucidate the influence of alginate chemical composition and molecular weight on the gel elasticity and molecular structure. The alginic acid gels were prepared by homogeneous pH reduction throughout the sample. Three alginates with different chemical composition and sequence, and two to three different molecular weights of each sample were examined. Three alginate samples with fractions of guluronic acid residues of 0.39 (LoG), 0.50 (InG), and 0.68 (HiG), covering the range of commercially available alginates, were employed. The excess scattering intensity I of the alginic acid gels was about 1 order of magnitude larger and exhibited a stronger curvature toward low q compared to ionically cross-linked alginate. The I(q) were decomposed into two components by assuming that the alginic acid gel is composed of aggregated multiple junctions and single chains. Time-resolved experiments showed a large increase in the average size of aggregates and their weight fraction within the first 2 h after onset of gelling, which also coincides with the most pronounced rheological changes. At equilibrium, little or no effect of molecular weight was observed, whereas at comparable molecular weights, an increased scattering intensity with increasing content of guluronic acid residues was recorded, probably because of a larger apparent molecular mass of domains. The results suggest a quasi-ordered junction zone is formed in the initial stage, followed by subsequent assembling of such zones, forming domains in the order of 50 A. The average length of the initial junction zones, being governed by the relative fraction of stabilizing G-blocks and destabilizing alternating (MG) blocks, determines the density of the final random aggregates. Hence, high-G alginates give alginic acid gels of a higher aggregate density compared to domains composed of loosely packed shorter junction zones in InG or LoG system.     

Conformations and interactions of pectins: II. Models for junction zones in pectinic acid and calcium pectate gels

Pectinic acid and calcium pectate gels condensed into uniaxially oriented fibers have been studied by X-ray diffraction. Although the diffraction patterns correspond to systems of only limited order, they show that both systems conserve the 1.3 nm axial period and 0.43 nm pseudo-period observed in sodium pectate. Pectinic acid further resembles sodium pectate in packing isometrically in a hexagonal net of side 0.84 nm. On the other hand, calcium pectate fibers contain the 1.2 nm lateral spacing observed in pectic acid. Speculative models for pectinic acid and calcium pectate have been developed. The former structure could be stabilized by hydrophobic binding from columns of methyl groups as well as by specific intermolecular hydrogen bonds. In the latter, the main interactions between pairs of chains could be bridges formed by calcium ions, which incorporate into their co-ordination shells two polyanion oxygen atoms from one chain and three from another. These model-building studies provide plausible visualizations of two different kinds of junction zones that may exist in pectic gels.     

A 13C CP/MAS NMR spectroscopy and AFM study of the structure of Glucagel™, a gelling β-glucan from barley

The structure of Glucagel™, a mixed-linked (1→3), (1→4)-β-d-glucan extracted from barley, was examined using ¹³C CP/MAS NMR spectroscopy and atomic force microscopy (AFM). Results from ¹³C CP/MAS NMR spectroscopy showed that Glucagel™ contained regions with two distinct conformations. In some of the regions the β-glucan chains associated to form a unique conformation, the A-conformation, while in the other regions the β-glucan chains were in an amorphous conformation. Dilute solutions of Glucagel™ were prepared for imaging by dissolving Glucagel™ in water at 90 °C. If the dilute solution was immediately deposited onto mica and the surface dried, then no fine detail was seen in the AFM image. However, when dilute solutions of Glucagel™ were left for several days before being deposited onto the mica surface, individual fibres could be clearly imaged. These results suggested that in gels formed from Glucagel™, junction zones occur because of the interaction of two β-glucan chains in the A-conformation.     

Structural characterisation of thermoreversible anionic polysaccharide gels by their elastoviscous properties

Previously reported results obtained for the elastoviscous properties of some thermoreversible gels formed from anionic polysaccharides (high methoxyl pectin, furcellaran and κ-carrageenan) and also gelatin and maltodextrin are discussed and some conclusions about the structure of the gels are presented.The rate at which the relaxation processes take place in the gel is independent of the polymer concentration suggesting that the gels are structurally inhomogeneous.If the helical conformation of the individual macromolecule is stable the standard enthalpy change on crosslink breakdown is less than 45 kJ mol^?1. A relatively small decrease in standard enthalpy is sufficient for network stability because of the low standard entropy loss on gelation which is typical of semi-rigid chain polymers. If, however, the helical conformation is unstable the gelation process is cooperative and the standard enthalpy change on crosslink breakdown exceeds 200 kJ mol^?1.     

The crystal and molecular structure of the alpha-helical nonapeptide antibiotic leucinostatin A

The crystal and molecular structure of the nonapeptide antibiotic leucinostatin A, containing some uncommon amino acids and three Aib residues, has been determined by x-ray diffraction analysis. The molecule crystallizes in the orthorhombic space group P2(1)2(1)2(1), a = 10.924, b = 17.810, c = 40.50 A, C62H111N11O13, HCl.H2O, Z = 4. The peptide backbone folds in a regular right-handed alpha-helix conformation, with six intramolecular i----(i + 4) hydrogen bonds, forming C13 rings. The nonapeptide chain includes at the C end an unusual beta-Ala residue, which also adopts the helical structure of the other eight residues. In the crystal the helices are linked head to tail by electrostatic and hydrogen-bond interactions, forming continuous helical rods. The crystal packing is formed by adjacent parallel and antiparallel helical rods. Between adjacent parallel helical columns there are only van der Waals contacts, while between adjacent antiparallel helical columns hydrogen-bond interactions are formed.     

Freely diffusing single hairpin ribozymes provide insights into the role of secondary structure and partially folded states in RNA folding

Single-molecule fluorescence resonance energy transfer studies of freely diffusing hairpin ribozymes with different combinations of helical junction and loop elements reveal striking differences in their folding behavior. We examined a series of six different ribozymes consisting of two-, three- and four-way junction variants, as well as corresponding constructs with one of the two loops removed. Our results highlight the varying contributions of preformed secondary structure elements to tertiary folding of the hairpin ribozyme. Of the three helical junction variants studied, the four-way junction strongly favored folding to a docked conformation of the two loops, required for catalytic activity. Moreover, the four-way junction was uniquely able to fold to a similar compact structure even in the absence of specific loop-loop docking interactions. A key feature of the data is the observation of broadening/tailing in the fluorescence resonance energy transfer histogram peak for a single-loop mutant of the four-way junction at higher Mg(2+) concentrations, not observed for any of the other single-loop variants. This feature is consistent with interconversion between compact and extended structures, which we estimate takes place on the 100-micros timescale using a simple model for the peak shape. This unique ability of the four-way junction ribozyme to populate an undocked conformation with native-like structure (a quasi-docked state) likely contributes to its greater tertiary structure stability, with the quasi-docked state acting as an intermediate and facilitating the subsequent formation of the specific hydrogen bonding network during docking of the two loops. The inability of two- and three-way junction ribozymes to fully populate a docked conformation reveals the importance of correct helical junction geometry as well as loop elements for effective ribozyme folding.     

Supramolecular assembly using helical peptides

We investigated supramolecular assemblies of various hydrophobic helical peptides. The assemblies were formed at the air/water interface or in aqueous medium. The hexadecapeptide, Boc-(Ala-Aib)₈-OMe (BA16M), was reported to take α-helical structure by X-ray analysis. Several derivatives were prepared, which have the repeating sequence of Ala-Aib, Lys(Z)-Aib or Leu-Aib, or have the terminal chemically modified. CD spectra of the peptides indicated helical conformation in ethanol solution. The surface pressure-area isotherms of the peptide monolayers showed an inflection at the surface area corresponding to the cross section along the helix axis, and the monolayers were collapsed by further compression. All the helical peptides oriented their helix axis parallel to the air/water interface on the basis of the results of transmission IR spectra and RAS of the monolayers transferred onto substrates.A small mound was observed in the isotherm of BA16M and other derivatives, which was ascribed to the phase transition from the liquid state to the solid state. One mol% of FITC-labeled peptide was mixed into the monolayers to visualize the phase separation of the solid and liquid states at the surface pressure of the coexisting region. Various shapes of the dark domain were observed at the top of the mound in the isotherms by fluorescence microscopy. The helical peptides formed two-dimensional crystals at the air/water interface when they were compressed to the solid state.An amino-terminated helical peptide, HA16B, was suspended in an aqueous medium by a sonication method and transparent dispersion was obtained. The dynamic light scattering measurement of the dispersion revealed the particle size of 75 nm with a narrow size distribution. The molecular assembly of the helical peptide in water was called “Peptosome”, because it takes a vesicular structure.     

Using SAXS to reveal the degree of bundling in the polysaccharide junction zones of microrheologically distinct pectin gels

The results of microrheological studies carried out on ionotropic pectin gels, particularly the manifest power law behavior observed at high frequencies, indicate that by using different assembly conditions gels can be formed in which the elementary network strands have different stiffnesses. It has been hypothesized that these differences reflect different network architectures, the extreme cases of which might be described as (i) dimeric calcium-chelating junction-zones of limited extent, linked by considerably longer, flexible, single-chain sections, or (ii) semiflexible bundles consisting of extensively aggregated dimeric junction zones that latterly become entangled and cross-linked. To test this hypothesis directly, microrheologically distinct pectin gels have been generated using different assembly modalities, in particular by using different concentrations of polymer and cross-linking ions and by contrasting the controlled-release of ions or ion-binding groups, and the resulting systems have been studied by small-angle X-ray scattering. The results straightforwardly reveal that gels that are clearly more semiflexible from a microrheological point-of-view contain larger scattering entities than those with a more flexible character. Furthermore, a more detailed interpretation of the scattering data with the aid of molecular modeling suggests that for the gels formed here those with a semiflexible microrheological signature consist predominantly of network filaments consisting of four or more chains, whereas those with a more flexible signature are predominantly single-chain sections linked by dimeric associations with no more that a few percent of the chains bundled to any higher extent. The ability to generate differing network architectures from the same polymer that fulfill different functional requirements, either in vivo in the plant cell wall, where pectin plays a crucial structural and mechanical role, or in vitro in a myriad of applications, makes these biomimetic biopolymer networks of considerable interest.     

Crystal and molecular structure of Boc-D-Ala-delta Phe-Gly-delta Phe- D-Ala-OMe: a 3 10-helical dehydropeptide

The crystal and molecular structure of the pentapeptide Boc-D-Ala-delta Phe-Gly-delta Phe-D-Ala-OMe, containing two dehydrophenylalanine residues, was determined by x-ray diffraction. The molecule crystallizes in the orthorombic P2(1)2(1)2(1) space group, with a = 10.439(3), b = 15.319(3) and c = 21.099(4) A. In the solid state, the conformation of the pentapeptide is characterized by the presence of two type III' beta-turns. Thus the peptide assumes a left-handed 3(10-helical conformation, the left sense being due to the D configuration of the alanine residues. The two unsaturated residues are located in the (i + 1) position of the first beta-turn and in the (i + 2) position of the second beta-turn, respectively. In the crystal, the helical molecules are linked head to tail by hydrogen bonds. Lateral hydrogen bonds are also formed between molecules related by a twofold screw symmetry. This gives rise to a typical mode of packing characterized by infinite helical "chains,' similar to the packing found in other oligopeptides that adopt a 3(10)-helical structure.     

Structural characteristics and rheological properties of partially hydrolyzed oat β-glucan: the effects of molecular weight and hydrolysis method

Partial hydrolysates of (1→3)(1→4)-β- -glucan from oats were produced by three hydrolysis methods: acid, cellulase or lichenase. The molecular weights ranged from 31 000 to 237 000 g/mol. Six percent solutions of small molecular weight β-glucans formed elastic gels after 4 days at 4 °C whereas larger molecular weight β-glucans remained viscous liquids after 7 days. The melting temperature of the gels increased as they aged and the peak heat flow temperature, measured by differential scanning calorimetry, was 62±2 °C. Partial hydrolysates produced with cellulase, which was shown to preferentially cleave regions of the molecule with longer contiguous β-(1→4)-linked -glucopyranosyl units, tended to produce more elastic gels with stronger junction zones than partial hydrolysates produced with lichenase which cleaves the β-(1→4) glycosidic 3-o-substituted glucose links. This suggests that β-(1→3)-linked cellotriose sections of the polymer are probably the segments which form the junction zones in the gel network rather than cellulose-like segments.     

斜顶菌水溶性多糖的构象研究

根据光散射法与粘度法对斜顶菌(Clitopilus Caespitosus PK)多糖在水中与在二甲亚砜中的分子量所进行的对比测定(3:1)以及由多糖水溶液可与刚果红形成络合物的实验结果,推测此多糖在水中是三股螺旋构象,而在DMSO中是单股螺旋。在H_2O—DMSO混合溶剂体系中,体积分数φH_2O降至0.18后,三股螺旋解体为单股螺旋,这种解离具有可逆性。变性剂如脲、酸、碱与高温等条件均因破坏氢键而影响构象的变化。用X射线粉末衍射,确定多糖具有规整有序并有重复性的空间结构。     

Type XIII collagen forms homotrimers with three triple helical collagenous domains and its association into disulfide-bonded trimers is enhanced by prolyl 4-hydroxylase

Type XIII collagen is a type II transmembrane protein predicted to consist of a short cytosolic domain, a single transmembrane domain, and three collagenous domains flanked by noncollagenous sequences. Previous studies on mRNAs indicate that the structures of the collagenous domain closest to the cell membrane, COL1, the adjacent noncollagenous domain, NC2, and the C-terminal domains COL3 and NC4 are subject to alternative splicing. In order to extend studies of type XIII collagen from cDNAs to the protein level we have produced it in insect cells by means of baculoviruses. Type XIII collagen alpha chains were found to associate into disulfide-bonded trimers, and hydroxylation of proline residues dramatically enhanced this association. This protein contains altogether eight cysteine residues, and interchain disulfide bonds could be located in the NC1 domain and possibly at the junction of COL1 and NC2, while the two cysteine residues in NC4 are likely to form intrachain bonds. Pepsin and trypsin/chymotrypsin digestions indicated that the type XIII collagen alpha chains form homotrimers whose three collagenous domains are in triple helical conformation. The thermal stabilities (T(m)) of the COL1, COL2, and COL3 domains were 38, 49 and 40 degrees C, respectively. The T(m) of the central collagenous domain is unusually high, which in the light of this domain being invariant in terms of alternative splicing suggests that the central portion of the molecule may have an important role in the stability of the molecule. All in all, most of the type XIII collagen ectodomain appears to be present in triple helical conformation, which is in clear contrast to the short or highly interrupted triple helical domains of the other known collagenous transmembrane proteins.     

Modular design of synthetic protein mimics. Characterization of the helical conformation of a 13-residue peptide in crystals

The incorporation of alpha-aminoisobutyryl (Aib) residues into peptide sequences facilitates helical folding. Aib-containing sequences have been chosen for the design of rigid helical segments in a modular approach to the construction of a synthetic protein mimic. The helical conformation of the synthetic peptide Boc-Aib-(Val-Ala-Leu-Aib)3-OMe in crystals is established by X-ray diffraction. The 13-residue apolar peptide adopts a helical form in the crystal with seven alpha-type hydrogen bonds in the middle and 3(10)-type hydrogen bonds at either end. The helices stack in columns, zigzag rather than linear, by means of direct NH...OC head to tail hydrogen bonds. Leucyl side chains are extended on one side of the helix and valyl side chains on the other side. Water molecules form hydrogen bonds with several backbone carbonyl oxygens that also participate in alpha-helix hydrogen bonds. There is no apparent distortion of the helix caused by hydration. The space group is P2(1)2(1)2(1), with a = 9.964 (3) A, b = 20.117 (3) A, c = 39.311 (6) A, Z = 4, and dx = 1.127 g/cm3 for C64H106N13O16.1.33H2O. The final agreement factor R was 0.089 for 3667 data observed greater than 3 sigma(F) with a resolution of 0.9 A.     

The complete VS ribozyme in solution studied by small-angle X-ray scattering

We have used small-angle X-ray solution scattering to obtain ab initio shape reconstructions of the complete VS ribozyme. The ribozyme occupies an electron density envelope with an irregular shape, into which helical sections have been fitted. The ribozyme is built around a core comprising a near-coaxial stack of three helices, organized by two three-way helical junctions. An additional three-way junction formed by an auxiliary helix directs the substrate stem-loop, juxtaposing the cleavage site with an internal loop to create the active complex. This is consistent with the current view of the probable mechanism of trans-esterification in which adenine and guanine nucleobases contributed by the interacting loops combine in general acid-base catalysis.     

Assembly and characterization of five-arm and six-arm DNA branched junctions.

DNA branched junctions have been constructed that contain either five arms or six arms surrounding a branch point. These junctions are not as stable as junctions containing three or four arms; unlike the smaller junctions, they cannot be shown to migrate as a single band on native gels when each of their arms contains eight nucleotide pairs. However, they can be stabilized if their arms contain 16 nucleotide pairs. Ferguson analysis of these junctions in combination with three-arm and four-arm junctions indicates a linear increase in friction constant as the number of arms increases, with the four-arm junction migrating anomalously. The five-arm junction does not appear to have any unusual stacking structure, and all strands show similar responses to hydroxyl radical autofootprinting analysis. By contrast, one strand of the six-arm junction shows virtually no protection from hydroxyl radicals, suggesting that it is the helical strand of a preferred stacking domain. Both junctions are susceptible to digestion by T4 endonuclease VII, which resolves Holliday junctions. However, the putative helical strand of the six-arm junction shows markedly reduced cleavage, supporting the notion that its structure is largely found in a helical conformation. Branched DNA molecules can be assembled into structures whose helix axes form multiply connected objects and networks. The ability to construct five-arm and six-arm junctions vastly increases the number of structures and networks that can be built from branched DNA components. Icosahedral deltahedra and 11 networks with 432 symmetry, constructed from Platonic and Archimedean solids, are among the structures whose construction is feasible, now that these junctions can be made.     

Small-angle X-ray scattering study of the (Fab′)2 fragment of the human immunoglobulin Kol

The conformation of the (Fab′)₂ fragment of the human immunoglubulin Kol has been investigated in solution by small angle X-ray scattering. The following molecular parameters were determined: radius of gyration 4.10 ± 0.05 nm; maximum distance 14.0 ± 0.5 nm and hydrated volume 150 ± 8 nm³. A model of the fragment is presented, which fits these experimental data and shows good agreement with the distance distribution function in real space and the scattering curve in reciprocal space. We have to assume that the (Fab′)₂ fragment has many different conformations in solution. The method of small-angle X-ray scattering only allows the determination of an average conformation which is very similar within the resolution of the method to the static structure determined in the crystal.     

Structure and conformation of peptides containing the sulphonamide junction. III. Synthesis, crystal and molecular structure of a taurine containing peptidic oxa-cyclol

The insertion of the (S)-lactyl residue into the cyclodipeptide cyclo (-Tau-Pro-) 3 leads in good yields to the first example of a stable tetrahedral adduct (oxa-cyclol) 5 containing the sulphonamide junction. Compound 5 does not show a significant tendency towards tautomeric equilibria and possesses an unexpected syn-orientation involving the hydroxyl group and the Pro-H alpha. The crystal structure and molecular conformation of 5 has been determined. Crystals are orthorhombic, s.g. P2(1)2(1)2(1), with a = 6.607, b = 12.297, c = 16.622 A. The cisoidal conformation around the S-N bond is very similar to that found in the previously studied linear and cyclic peptides containing a sulphonamide junction. The taurine nitrogen is practically planar whereas the proline nitrogen, bound to the SO2 group, is highly pyramidal. In the tricyclic system of 5 the seven-membered ring adopts a twist-chair conformation while the pyrrolidine and oxazolidinone rings show an envelope conformation. The crystal packing is characterized by three hydrogen bonds all formed by means of a water molecule.     

Refinement of the solution structure of a branched DNA three-way junction.

We have refined the structure of the DNA Three-Way Junction complex, TWJ-TC, described in the companion paper by quantitative analysis of two 2D NOESY spectra (mixing times 60 and 200 ms) obtained in D2O solution. NOESY crosspeak intensities extracted from these spectra were used in two kinds of refinement procedure: 1) distance-restrained energy minimization (EM) and molecular dynamics (MD) and 2) full relaxation matrix back calculation refinement. The global geometry of the refined model is very similar to that of a published, preliminary model (Leontis, 1993). Two of the helical arms of the junction are stacked. These are Helix 1, defined by basepairs S1-G1/S3-C12 through S1-C5/S3-G8 and Helix 2, which comprises basepairs S1-C6/S2-G5 through S1-G10/S2-G1. The third helical arm (Helix 3), comprised of basepairs S2-C6/S3-G5 through S2-C10/S3-G1 extends almost perpendicularly from the axis defined by Helices 1 and 2. The bases S1-C5 and S1-C6 of Strand 1 are continuously stacked across the junction region. The conformation of this strand is close to that of B-form DNA along its entire length, including the S1-C5 to S1-C6 dinucleotide step at the junction. The two unpaired bases S3-T6 and S3-C7 lie outside of the junction along the minor groove of Helix 1 and largely exposed to solvent. Analysis of the refined structure reveals that the glycosidic bond of S3-T6 exists in the syn conformation, allowing the methyl group of this residue to contact the hydrophobic surface of the minor groove of Helix 1, at S3-G11.(ABSTRACT TRUNCATED AT 250 WORDS)     

Molecular and crystal structures of chitosan/HI type I salt determined by X-ray fiber diffraction

The three-dimensional structure of chitosan/HI type I salt was determined by the X-ray fiber diffraction technique and linked-atom least-squares refinement method. Two polymer chains and four iodide ions (I(-)) crystallized in a monoclinic unit cell with dimensions a = 9.46(2), b = 9.79(2)], c (fiber axis)=10.33(2)A, beta = 105.2(2) degrees and a space group P2(1). Chitosan chains adopted an extended twofold helical conformation that was stabilized by O-3...O-5 hydrogen bonds, and the O-6 atom adopted nearly gt orientation. Polymer chains zigzag along the b-axis and directly connect to each other by N-2...O-6 hydrogen bonds. Two columns of iodide ions were shown to pack at the bending points of the zigzag sheets, and their locations are closely related to those of water columns in the hydrated chitosan. The iodide ions stabilized the salt structure by forming hydrogen bonds with the N-2 and O-6 atoms of the polymer chains together with an electrostatic interaction between N-2 and the iodide ions.