Influence of oligoguluronates on alginate gelation, kinetics, and polymer organization

Structural polysaccharides of the alginate family form gels in aqueous Ca2+-containing solutions by lateral association of chain segments. The effect of adding oligomers of alpha-l-guluronic acid (G blocks) to gelling solutions of alginate was investigated using rheology and atomic force microscopy (AFM). Ca-alginate gels were prepared by in situ release of Ca2+. The gel strength increased with increasing level of calcium saturation of the alginate and decreased with increasing amount of free G blocks. The presence of free G blocks also led to an increased gelation time. The gel point and fractal dimensionalities of the gels were determined based on the rheological characterization. Without added free G blocks the fractal dimension of the gels increased from df = 2.14 to df = 2.46 when increasing [Ca2+] from 10 to 20 mM. This increase was suggested to arise from an increased junction zone multiplicity induced by the increased concentration of calcium ions. In the presence of free G blocks (G block/alginate = 1/1) the fractal dimension increased from 2.14 to 2.29 at 10 mM Ca2+, whereas there was no significant change associated with addition of G blocks at 20 mM Ca2+. These observations indicate that free G blocks are involved in calcium-mediated bonds formed between guluronic acid sequences within the polymeric alginates. Thus, the added oligoguluronate competes with the alginate chains for the calcium ions. The gels and pregel situations close to the gel point were also studied using AFM. The AFM topographs indicated that in situations of low calcium saturation microgels a few hundred nanometers in diameter develop in solution. In situations of higher calcium saturation lateral association of a number of alginate chains are occurring, giving ordered fiber-like structures. These results show that G blocks can be used as modulators of gelation kinetics as well as local network structure formation and equilibrium properties in alginate gels.     

Structure of the vanadate-induced crystals of sarcoplasmic reticulum Ca2+-ATPase

The projected structure of the vanadate-induced crystalline aggregates of Ca2+-ATPase molecules in isolated sarcoplasmic reticulum membranes has been determined. The molecules form tubular crystals with an oblique surface lattice having cell dimensions a = 65.9 A, b = 114.4 A and gamma = 77.9 degrees. The space group is P2. The crystalline tubules are formed through lateral aggregation of chains made up of dimers of Ca2+-ATPase molecules.     

A small-angle x-ray scattering study of alginate solution and its Sol–Gel transition by addition of divalent cations

The small-angle x-ray scattering (SAXS) technique has been applied to investigate solution and gel structures of alginate in the absence and presence of two divalent cations: Ca(II) and Cu(II). We have observed a broad maximum in the scattering curve, a characteristic of polyelectrolyte, for the purified alginate sample. The scattering maximum disappears in excess of added simple salt and shifts toward the higher angle region with increasing alginate concentration. Concentration dependence of the position and intensity of the maximum follows power law relations with exponents close to those predicted by theory. Data analysis shows an increase in correlation length ξ and cross-sectional diameter d₀, of polymer chains upon gelation and suggests that a dimeric structure is adopted in the junction zone, consistent with the “egg-box” model previously proposed. In the Ca(II)–alginate system, the molecular parameters ξ and d₀ are found to have good correlation with the macroscopic properties of gelation, such as gel point determined by viscosity measurements. However, for the Cu(II)–alginate system there is no clearly transitional behavior observed in ξ and d₀, implying that the junction zone may be replaced by a more uniformly distributed site binding of Cu(II) ions to the carboxyl groups of both mannuronate and guluronate residues, in confirmation of previous ¹³C-nmr results. © 1995 John Wiley & Sons, Inc.     

Formation of a hexagonal lattice structure by an R-form lipopolysaccharide of Klebsiella: effect of various divalent cations on the lattice formation

The R-form lipopolysaccharide from Klebsiella pneumoniae strain LEN-111 (O3-:K1-), from which cationic material had been removed by electrodialysis, was previously shown to form a hexagonal lattice structure with the lattice constant of 14 to 15 nm when suspended in 50 mM tris(hydroxymethyl)aminomethane buffer at pH 8.5 containing 10 mM Mg2+. Under this experimental condition, effects of other divalent metal cations on the hexagonal assembly of the electrodialyzed LPS were compared with that of Mg2+. The Zn2+, Hg2+, Cu2+, and Ni2+ could produce essentially the same hexagonal lattice structure with the lattice constant of 14.5 to 15.0 nm as that formed with Mg2+. The Cd2+, Co2+, and Fe2+ produced the hexagonal lattice structure with the lattice constant of 15.5 to 16.0 nm, and Ba2+, Sr2+, and Ca2+ produced that with the lattice constant of 18 to 19 nm. In addition, the hexagonal lattice structures formed with the latter three cations were less orderly than those formed with the other cations. When the higher concentrations of Ba2+, Sr2+, and Ca2+ were used, the lattice constants were not shortened. The length of lattice constants of the hexagonal lattice structures formed with the divalent cations did not relate to the quantity of the cations bound to the LPS. Among the divalent cations tested, Hg2+ was bound to the LPS in the smallest amount (its atomic ratio to P, 0.07), and Zn2+ and Fe2+ were bound in very large amounts (their atomic ratios to P, 2.94 and 8.28, respectively).     

New insights into the mechanism of gelation of alginate and pectin: charge annihilation and reversal mechanism

Studies have been undertaken on the binding of Mn2+ ions to two alginate samples of different mannuronate:guluronate ratios (M:G), a sample of low-ester amidated pectin and poly(acrylic acid) (PAA). The binding of Ca2+ ions has also been included for the latter for comparison. The binding curves showed an initial steep rise at low additions of Mn2+ or Ca2+ indicating that all of the ions were bound to the polymer chains with none remaining in solution. At higher additions, the binding curves showed a plateau region and the maximum amount bound, theta, was found to be 0.2, 0.2, 0.25, and 0.33 mol M(2+)/mol COO- for high M:G alginate, low M:G alginate, pectin, and PAA, respectively. The binding curves for Mn2+ and Ca2+ with PAA were superimposable. In all cases, theta was less than the stoichiometric equivalent and also less than predicted by Manning counterion condensation theory. The linear charge density, xi, for the polymers is 1.49, 1.55, 1.62, and 2.85, and it was found that at maximum binding the effective linear charge density, xi(effective), decreased to a value close to 1 in each case and not 0.5 as predicted from Manning's two-variable theory. The mobility of the PAA chains has been followed by electron spin resonance spectroscopy using nitroxide spin labels covalently attached to the polymer, and the gelation of the pectin and alginate samples has been monitored using small deformation oscillatory experiments. For PAA at maximum binding, it was noted that there was a loss of chain mobility and precipitation. For pectin and alginate, gelation occurred and the stoichiometric ratio for maximum binding corresponded to the stoichiometric ratio for the maximum in G'. Precipitation and gelation are attributed to the formation of polymer-metal complexes involving one or two carboxylate groups resulting in charge reversal or charge annihilation.     

The structure of the Ca2+ ATPase as revealed by electron microscopy and image processing of ordered arrays

Two-dimensional ordered arrays of the membrane-bound Ca2+ ATPase, were formed over a wide range of conditions (i.e., pH, ionic strength, temperature) in the presence of vanadate, and studied by electron microscopy and image processing. These ordered tubular and spherical membrane vesicles of Ca2+ ATPase could also be formed with approximately one bound ATP and between one and two nonchelatable Ca2+ bound. The tubular arrays ranged between 1 and 10 microns in length and had an average flattened diameter of 90 nm, as observed in negatively stained preparations. The basic building blocks of these ordered arrays appear to be linear ribbons of Ca2+ ATPase dimers. Fourier analysis of electron micrographs of these flattened tubes revealed a near-rectangular lattice (lattice angle 73.3 +/- 4.6 degrees with average lattice constants of a = 6.2 +/- 0.25 nm, and b = 11.5 +/- 0.30 nm). The double-stranded ribbons (i.e., parallel to a) are inclined by 56 +/- 3.7 degrees relative to the tube axis in a right-handed sense, as determined from freeze-dried metal-shadowed specimens. Computer averaging of negatively stained arrays reveals a crystallographic dimer of stain-excluding matter. The dimensions of each monomer within this dimer are consistent with established structural parameters, leading us to believe a form of the Ca2+ ATPase, capable of binding at least one ATP and of binding Ca2+ ions, may exist as a dimer in the sarcoplasmic reticulum.     

Factors affecting the dissociation and aggregation of human interferon gamma

The biologically active form of interferon γ (IFN-γ) is a dimer consisting of two identical non-covalently bound polypeptide chains. We have studied spectroscopically the dimer–monomer dissociation equilibrium of human recombinant IFN-γ and have found that the monomers possess approximately 50% lower Trp quantum yield than the dimers [Boteva et al. Biochemistry 1996;35:14825]. In the present study we characterise the conformational properties of the two states — monomeric and dimeric, and analyse the effects of the salt composition of human blood plasma, physiological cations K⁺, Na⁺, Ca²⁺ and Mg²⁺ and mechanical stress on the dimer–monomer equilibrium. A medium with electrolyte composition of human blood plasma increases both the association and dissociation rate constants without shifting significantly the dimer–monomer equilibrium. The physiological cations shift the equilibrium towards dissociation of dimers into monomers by lowering the activation energy and the free energy of the process thus decreasing the stability of IFN-γ. Mechanical stress caused by stirring of the protein solution reduces irreversibly the Trp fluorescence by 75–80% and decreases significantly the -helical content and favours the aggregation.     

Order-disorder structural transitions in synthetic filaments of fast and slow skeletal muscle myosins under relaxing and activating conditions

In the previous study (Podlubnaya et al., 1999, J. Struc. Biol. 127, 1-15) Ca2+-induced reversible structural transitions in synthetic filaments of pure fast skeletal and cardiac muscle myosins were observed under rigor conditions (-Ca2+/+Ca2+). In the present work these studies have been extended to new more order-producing conditions (presence of ATP in the absence of Ca2+) aimed at arresting the relaxed structure in synthetic filaments of both fast and slow skeletal muscle myosin. Filaments were formed from column-purified myosins (rabbit fast skeletal muscle and rabbit slow skeletal semimebranosusproprius muscle). In the presence of 0.1 mM free Ca2+, 3 mM Mg2+ and 2 mM ATP (activating conditions) these filaments had a spread structure with a random arrangement of myosin heads and subfragments 2 protruding from the filament backbone. Such a structure is indistinguishable from the filament structures observed previously for fast skeletal, cardiac (see reference cited above) and smooth (Podlubnaya et al., 1999, J. Muscle Res. Cell Motil. 20, 547-554) muscle myosins in the presence of 0.1 mM free Ca2+. In the absence of Ca2+ and in the presence of ATP (relaxing conditions) the filaments of both studied myosins revealed a compact ordered structure. The fast skeletal muscle myosin filaments exhibited an axial periodicity of about 14.5 nm and which was much more pronounced than under rigor conditions in the absence of Ca2+ (see the first reference cited). The slow skeletal muscle myosin filaments differ slightly in their appearance from those of fast muscle as they exhibit mainly an axial repeat of about 43 nm while the 14.5 nm repeat is visible only in some regions. This may be a result of a slightly different structural properties of slow skeletal muscle myosin. We conclude that, like other filaments of vertebrate myosins, slow skeletal muscle myosin filaments also undergo the Ca2+-induced structural order-disorder transitions. It is very likely that all vertebrate muscle myosins possess such a property.     

Localization and characterization of the inhibitory Ca2+-binding site of Physarum polycephalum myosin II

A myosin II is thought to be the driving force of the fast cytoplasmic streaming in the plasmodium of Physarum polycephalum. This regulated myosin, unique among conventional myosins, is inhibited by direct Ca2+ binding. Here we report that Ca2+ binds to the first EF-hand of the essential light chain (ELC) subunit of Physarum myosin. Flow dialysis experiments of wild-type and mutant light chains and the regulatory domain revealed a single binding site that shows moderate specificity for Ca2+. The regulatory light chain, in contrast to regulatory light chains of higher eukaryotes, is unable to bind divalent cations. Although the Ca2+-binding loop of ELC has a canonical sequence, replacement of glutamic acid to alanine in the -z coordinating position only slightly decreased the Ca2+ affinity of the site, suggesting that the Ca2+ coordination is different from classical EF-hands; namely, the specific "closed-to-open" conformational transition does not occur in the ELC in response to Ca2+. Ca2+- and Mg2+-dependent conformational changes in the microenvironment of the binding site were detected by fluorescence experiments. Transient kinetic experiments showed that the displacement of Mg2+ by Ca2+ is faster than the change in direction of cytoplasmic streaming; therefore, we conclude that Ca2+ inhibition could operate in physiological conditions. By comparing the Physarum Ca2+ site with the well studied Ca2+ switch of scallop myosin, we surmise that despite the opposite effect of Ca2+ binding on the motor activity, the two conventional myosins could have a common structural basis for Ca2+ regulation.     

Difference in concentration dependence of relaxation critical exponent N for alginate solutions at sol-gel transition induced by calcium cations

The sol-gel transition in aqueous alginate solutions induced by chelation with calcium cations from in situ release has been investigated with viscoelastic methods. Two alginate samples having different molecular weights (MW) were used over the concentration C(Alg) of 2 approximately 6 wt % with different mole ratio f of Ca2+ to the alginate repeat unit. The gel point f(gel) and relaxation critical exponent n were determined according to Winter's criterion, the later agrees well with that obtained from the relaxation modulus. The results indicate that the power law is valid for the dynamic relaxation at the gel point and the critical gel possesses the self-similarity in structure. With increasing C(Alg), f(gel) for the alginate with lower MW decreases dramatically and n is almost constant of about 0.71. In contrast, f(gel) for the higher MW alginate with is almost a constant and n decreases from 0.72 then levels off at 0.37 with increasing C(Alg), indicating that the concentration dependence of n varies with MW of alginate in the starting solution. The fractal dimension d(f) estimated from n suggests a denser structure in the critical gel of higher MW alginate. Either n or d(f) has been found to follow one curve for the two samples if plotted against the number of cross-link junctions per polymer chain, which is proportional to the alginate MW.     

Isolation, purification and partial characterization of a 30-kDa chlorophyll-a/b-binding protein from spinach

A 30-kDa chlorophyll-a/b-binding protein was purified from photosystem II membrane fragments using Ca(2+)-chelating Sepharose 6B chromatography. The protein binds approximately four chlorophyll a molecules, one chlorophyll b molecule and carotenoids. Its 77-K fluorescence-emission spectrum exhibits a maximum at 680 +/- 1 nm. The protein has a high tendency to form a dimer in the presence of Ca2+.Ca2+ binding affects the low-temperature fluorescence-emission maximum, leading to a decrease in its intensity and a blue shift of 1 nm. Similar spectral changes were obtained in the presence of Mg2+, possibly indicating a common binding domain for both cations. We interpret these observations as cation-induced conformational changes of the protein, which were reversible upon subsequent incubation in EDTA. Evidence is presented for the involvement of carboxyl groups in the coordination sphere of the bivalent cations. The possible structural and functional role of the protein is discussed.     

Calcium-dependent alpha-helical structure in osteocalcin

Osteocalcin is an abundant Ca2+-binding protein of bone containing three residues of vitamin K dependent gamma-carboxyglutamic acid (Gla) among its 49 (human, monkey, cow) or 50 (chicken) amino acids. Gla side chains participate directly in the binding of Ca2+ ions and the adsorption of osteocalcin to hydroxylapatite (HA) surfaces in vivo and in vitro. Osteocalcin exhibits a major conformational change when Ca2+ is bound. Metal-free chicken osteocalcin is a random coil with only 8% of its residues in the alpha helix as revealed by circular dichroism. In the presence of physiological levels of Ca2+, 38% of the protein adopts the alpha-helical conformation with a transition midpoint at 0.75 mM Ca2+ in a rapid, reversible fashion which (1) requires an intact disulfide bridge, (2) is proportionally diminished when Gla residues are decarboxylated to Glu, (3) is insensitive to 1.5 m NaCl, and (4) can be mimicked by other cations. Tyr fluorescence, UV difference spectra, and Tyr reactivity to tetranitromethane corroborate the conformational change. Homologous monkey osteocalcin also exhibits Ca2+-dependent structure. Integration of predictive calculations from osteocalcin sequence has yielded a structural model for the protein, the dominant features of which include two opposing alpha-helical domains of 9-12 residues each, connected by a bea turn and stabilized by the Cys23-Cys29 disulfide bond. Cation binding permits realization of the full alph a-helical potential by partial neutralization of high anionic charge in the helical domains. Periodic Gla occurrence at positions 17, 21, and 24 has been strongly conserved throughout evolution and places all Gla side chains on the same face of one alpha helix spaced at intervals of approximately 5.4 A, closely paralleling the interatomic separation of Ca2+ in the HA lattice. Helical osteocalcin has greatly increased affinity for HA; thus, the Ca2+-induced structural transition may perform an informational role related to bone metabolism.     

Proton and divalent cations induce synergistic but mechanistically different destabilizations of pH-sensitive liposomes composed of dioleoyl phosphatidylethanolamine and oleic acid

Protons and divalent cations show synergistic effects on the destabilization of liposomes composed of unsaturated phosphatidylethanolamine and oleic acid (Düzgünes et al., Biochemistry (1985) 24, 3091). We have extended these observations and investigated the effects of Ca2+ and Mg2+ on the proton-induced destabilization of dioleoyl phosphatidylethanolamine/oleic acid (DOPE/OA) (4:1 molar ratio) liposomes. Temperature-induced aggregation was measured by 90 degrees light scattering. Lipid mixing was used to monitor vesicle destabilization and freeze-fracture electron microscopy was used to examine the structures formed from DOPE/OA vesicles in the presence of Ca2+ and/or protons. Both Mg2+ and Ca2+ shift the pH required for 50% lipid mixing to higher values. Temperature-induced vesicle aggregation occurs at lower temperatures in the presence of divalent cations and/or protons, indicating that intervesicular repulsions are decreased. Freeze-fracture electron micrographs show that the structures formed from DOPE/OA in the presence of Ca2+ differ significantly from those found in the presence of protons. In general, protons induce the formation of hexagonal phase, while the presence of Ca2+ leads to the formation of extensive regions of lamellar sheets with numerous lipidic particles. The synergistic effect of divalent cations and proton may be important for the maximal biological activity of DOPE/OA liposomes.     

Binding of methylene blue to alginate: Effect of acid treatment on metachromasy

The spectral properties of methylene blue (MB) in solutions of Na alginate depend on the severity of prior acid treatment of the polysaccharide. The spectral properties affected are the fraction of MB in monomeric form, the relative amounts of metachromatic dye absorbing near 570 and near 595 nm, and the intensity and sign of circular dichroism (CD) activity associated with the 570 nm bands, at various ratios of polymer equivalents to dye (P/D) from 1300 to 4. Acid treatment consisted of reaction of dry, alcohol-precipitated and presumably native alginate with 0·3m HCl at room temperature for 5 min to 8 h. Acid-induced changes showed immediate (5 min) and slow (4–8 h) stages. In both stages the fractions of MB in monomeric form and in the 595 nm metachromatic form increased. CD activity was little affected by brief acid treatment (except in range P/D=165 to 55), but diminished at all P/D values on prolonged acid treatment. Minor changes were observed in the infrared spectra of alginate films. Fresh alcohol-precipitated alginate, untreated with acid, did not precipitate when dye was in excess, nor did it form gel beads in CaCl₂ solution. It is concluded that dilute acid treatment alters the stereospecific properties of native alginate, perhaps by inducing conformational changes in the constituent copolymer segments.     

Structure of the Azotobacter vinelandii surface layer.

Electron microscopy of the Azotobacter vinelandii tetragonal surface array, negatively stained with ammonium molybdate in the presence of 1 mM calcium chloride, showed an apparent repeat frequency of 12 to 13 nm. Image processing showed dominant tetrad units alternating with low-contrast cruciform structures formed at the junction of slender linkers extending from corner macromolecules of four adjoining dominant units. The actual unit cell showed p4 symmetry, and a = b = 18.4 nm. Distilled water extraction of the surface array released a multimeric form of the single 60,000 molecular-weight protein (S protein) which constitutes the surface layer. The molecular weight of the multimer was estimated at 255,000 by gel filtration, indicating a tetrameric structure of four identical subunits and suggesting that this multimer was the morphological subunit of the S layer. Tetrameric S protein exhibited low intrinsic stability once released from the outer membrane, dissociating into monomers when incubated in a variety of buffers including those which served as the base for defined media used to cultivate A. vinelandii. The tetramer could not be stabilized in these buffers at any temperature between 4 and 30 degrees C, but the addition of 2 to 5 mM Ca2+ or Mg2+ completely prevented its dissociation into monomers. Circular dichroism measurements indicated that the secondary structure of the tetramer was dominated by aperiodic and beta-sheet conformations, and the addition of Ca2+ did not produce any gross changes in this structure. Only the tetrameric form of S protein was able to reassemble in vitro in the presence of divalent cations onto the surface of cells stripped of their native S layer.     

Calcium ions are involved in the unusual red shift of the light-harvesting 1 Qy transition of the core complex in thermophilic purple sulfur bacterium Thermochromatium tepidum

Thermophilic purple sulfur bacterium, Thermochromatium tepidum, can grow at temperatures up to 58 degrees C and exhibits an unusual Qy absorption at 915 nm for the core light-harvesting complex (LH1), an approximately 35-nm red shift from those of its mesophilic counterparts. We demonstrate in this study, using a highly purified LH1-reaction center complex, that the LH1 Qy transition is strongly dependent on metal cations and Ca2+ is involved in the unusual red shift. Removal of the Ca2+ resulted in formation of a species with the LH1 Qy absorption at 880 nm, and addition of the Ca2+ to the 880-nm species recovered the native 915-nm form. Interchange between the two forms is fully reversible. Based on spectroscopic and isothermal titration calorimetry analyses, the Ca2+ binding to the LH1 complex was estimated to occur in a stoichiometric ratio of Ca2+/alphabeta-subunit = 1:1 and the binding constant was in 10(5) m(-1) order of magnitude, which is comparable with those for EF-hand Ca2+-binding proteins. Despite the high affinity, conformational changes in the LH1 complex upon Ca2+ binding were small and occurred slowly, with a typical time constant of approximately 6 min. Replacement of the Ca2+ with other metal cations caused blue shifts of the Qy bands depending on the property of the cations, indicating that the binding site is highly selective. Based on the amino acid sequences of the LH1 complex, possible Ca2+-binding sites are proposed that consist of several acidic amino acid residues near the membrane interfaces of the C-terminal region of the alpha-polypeptide and the N-terminal region of the beta-polypeptide.     

Specific interactions of divalent metal ions with a DNA duplex containing the d(CA)n/(GT)n tandem repeat

Divalent metal ions are essential for maintaining functional states of the DNA molecule. Their participation in DNA structure is modulated by the base sequence and varies depending on the nature of the ion. The present investigation addresses the interaction of Ca2+ ions with a tandem repeat of two CA dinucleotides, (CA)2/(TG)2. The binding of Ca2+ to the repeat is monitored by nuclear magnetic resonance (NMR) spectroscopy using chemical shift mapping. Parallel experiments monitor binding of Mg2+ ions to the repeat as well as binding of each ion to a DNA duplex in which the (CA)2/(TG)2 repeat is eliminated. The results reveal that the direction and the magnitude of chemical shift changes induced by Ca2+ ions in the NMR spectra of the repeat are different from those induced by Mg2+ ions. The differences between the two cations are significantly diminished by the elimination of the (CA)2/(TG)2 repeat. These findings suggest a specific interaction of Ca2+ ions with the (CA)2/(TG)2 motif. The specificity of the interaction resides in the two A-T base pairs of the repeat, and it involves the major groove of the first A-T base pair and both grooves of the second A-T base pair.     

Coordinated intercellular calcium waves induced by noradrenaline in rat hepatocytes: dual control by gap junction permeability and agonist.

Calcium-mobilizing agonists induce intracellular Ca2+ concentration ([Ca2+]i) changes thought to trigger cellular responses. In connected cells, rises in [Ca2+]i can propagate from cell to cell as intercellular Ca2+ waves, the mechanisms of which are not elucidated. Using fura2-loaded rat hepatocytes, we studied the mechanisms controlling coordination and intercellular propagation of noradrenaline-induced Ca2+ signals. Gap junction blockade with 18 alpha-glycyrrhetinic acid resulted in a loss of coordination between connected cells. We found that second messengers and [Ca2+]i rises in one hepatocyte cannot trigger Ca2+ responses in connected cells, suggesting that diffusion across gap junctions, while required for coordination, is not sufficient by itself for the propagation of intercellular Ca2+ waves. In addition, our experiments revealed functional differences between noradrenaline-induced Ca2+ signals in connected hepatocytes. These results demonstrate that intercellular Ca2+ signals in multicellular systems of rat hepatocytes are propagated and highly organized through complex mechanisms involving at least three factors. First, gap junction coupling ensures coordination of [Ca2+]i oscillations between the different cells; second, the presence of hormone at each hepatocyte is required for cell-cell Ca2+ signal propagation; and third, functional differences between adjacent connected hepatocytes could allow a 'pacemaker-like' intercellular spread of Ca2+ waves.     

Phase separation in calcium alginate gels

Alginates are polysaccharides consisting of beta-D-mannuronate and alpha-L-guluronate units. In the presence of bivalent cations like calcium the guluronate blocks form physically cross-linked gels. The gelation properties of alginates play an important role in the stability of extracellular polymer substances and in the food industry. When stock solutions of Ca2+ ions and alginate are mixed, the gelation starts before the Ca2+ ions are evenly distributed, which leads to non-uniform gels. In this contribution, Ca alginate gels were prepared by in situ gelation using glucono-delta-lactone and CaCO3. In this way, uniform gels could be prepared directly in the measuring cell. Below a critical concentration, highly viscous solutions were obtained, which were below the critical point of gel formation. In these solutions at low rotational speeds a Schlieren peak arose, which became smaller and steeper with increasing time until a new meniscus could be detected. This behaviour is in contrast to the peak broadening due to diffusion after a synthetic boundary was formed. Evaluation of the data leads to negative diffusion coefficients. It has been shown by others that the mutual diffusion coefficient must be negative in the spinodal region. This phenomena is known as uphill diffusion and leads to phase separation of a binary system. The formation of the gel phase in this case is therefore discussed as uphill diffusion.     

Arrangement of tubulin subunits and microtubule-associated proteins in the central-pair microtubule apparatus of squid (Loligo pealei) sperm flagella

This study provides a comprehensive, high-resolution structural analysis of the central-pair microtubule apparatus of sperm flagella. It describes the arrangement of several microtubule-associated "sheath" components and suggests, contrary to previous thinking, that microtubules are structurally asymmetric. The two microtubules of the central pair are different in several respects: the C2 tubule bears a single row of 18-nm-long sheath projections with an axial periodicity of 16 nm, whereas the C1 tubule possesses rows of 9-nm globular sheath components with an axial repeat of 32 nm. The lumen of the C2 tubule always appears completely filled with electron-dense material; that of the C1 tubule is frequently hollow. The C2 tubule also possesses a series of beaded chains arranged around the microtubule; the beaded chains are composed of globular subunits 7.5-10 nm in diameter and appear to function in the pairing of the C1 and C2 tubules. These findings indicate: that the beaded chains are not helical, but assume the form of lock washers arranged with a 16-nm axial periodicity on the microtubule; and that the lattice of tubulin dimers in the C2 tubule is not helically symmetric, but that there are seams between certain pairs of protofilaments. Proposed lattice models predict that, because of these seams, central pair and perhaps all singlet microtubules may contain a ribbon of 2-5 protofilaments that are resistant to solubilization; these models are supported by the results of the accompanying paper (R. W. Linck, and G. L. Langevin. 1981. J. Cell Biol. 89: 323-337.