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G Trombetta

Publications and source records attributed to G Trombetta.

At least 37 records · Page 2Linked to original sources

The osmotic properties and free energy of formation of the actomyosin rigor complexes from rabbit muscle.

We have studied the osmotic properties of the calcium-regulated actomyosin complexes from skeletal muscle at the protein osmotic pressure of 18 kPa and a different actin-to-myosin molar ratios. Essentially, protein solutions were equilibrated against a solution of poly(ethylene glycol) 40,000 of known macromolecular osmotic pressure. At the end of the equilibration the water and the protein masses of the protein solutions were determined gravimetrically and the protein molar concentration was calculated. In this reconstructed system we have found following, at the actin-to-molar ratio of 2.6 (the most likely stoichiometry of these two proteins in the dense region of the A band) the average distance between the myosin filaments is 34.2 nm, this equals the interfilament distance in the intact fibre of muscle in rigor, at the sarcomere length of 3.38 micrograms. The formation of the F-actin-myosin and of the tropomyosin-F-actin-myosin rigor complexes involves the largest free energy changes, -5.38 kJ/mol myosin and -5.67 kJ/mol myosin, respectively. The formation of the troponin-tropomyosin-F-actin-myosin(Ca) rigor complex from myosin and troponin-tropomyosin-F-actin(Ca) occurs with the free energy change of -3.43 kJ/mol myosin. Of these -3.43 kJ, -1.81 kJ are provided by the endergonic conversion of troponin-tropomyosin-F-actin(EGTA) into troponin-tropomyosin-F-actin (Ca). The transition of myosin and of troponin-tropomyosin-F-actin(EGTA) into the -F-actin-myosin(Ca) rigor complex is accompanied by a 5.8% increase of volume. The increase of volume is due to a large influx of water, which is essentially protein-hydration water.

Actins↗

The stiffness of the crossbridge is a function of the intrinsic protein osmotic pressure generated by the crossbridge itself.

A model is presented that makes it possible to determine the stiffness of the crossbridge from protein osmotic stress experiments. The model was elaborated while studying the osmotic properties of F-actin and of myosin subfragment-1 F-actin. These studies showed that the elastic modulus by bending of the monomer is directly related to the intrinsic protein osmotic pressure of the system. At a protein osmotic pressure of 1.8 x 10(5) dynes/cm2, the physiological protein osmotic pressure of frog skeletal muscle, it was found that the elastic moduli by bending of the monomer in F-actin and in the myosin subfragment-1 decorated F-actin are 6.5 X 10(7) and 3.3 X 10(8) dynes/cm2, respectively. The value of the elastic modulus by bending of the monomer in the myosin subfragment-1 decorated F-actin compares favorably with the values of the elastic modulus by stretching determined in skeletal muscle fibres.

Actins↗

Osmotic properties of myosin subfragment 1: implications of the mechanism of muscle contraction.

The osmotic behavior of myosin subfragment 1 was studied at 22 degrees C and pH 7.45 in 0.1 m KCl, 2 mm MgCl2, and 10 mm triethanolamine or in 25 mm phosphate, 2 mm MgCl2, and 2 mm MgADP. It was found that, in 0.1 m KCl, myosin subfragment 1 behaved as a spheroidal particle, with an average diameter of 8.09 nm, composed of two myosin subfragment 1 molecules. The lower limit of the thermodynamic dimerization constant was estimated to be 3.5 x 10(4) M-1. Above 5 mm as monomer, myosin subfragment 1 departed from the behavior expected of a dimeric spheroidal model because of the onset of a "hydration force." This force measured at the contact distance between particles equals 2.18 x 10(7) dynes/cm2 and falls off exponentially with a decay distance of 0.27 nm. In 25 mm orthophosphate, myosin subfragment 1, with an increase in the protein osmotic pressure, shifted from the behavior of a sphere to that of a cylinder. Between 1 x 10(5) and 4 x 10(5) dynes/cm2, the behavior of myosin subfragment 1 was different in the presence and in the absence of MgADP. In particular, at 1.8 x 10(5) dynes/cm2, the protein osmotic pressure in frog muscle, myosin subfragment 1 behaved as a sphere of 3.21-nm radius in the presence of MgADP and as a cylinder with a length to diameter ratio of 2.07 in the absence of MgADP. Under the solution conditions used in this work, S1 never behaved as a fully extended particle.

Adenosine Diphosphate↗

The "in vitro motility assay" and phalloidin-F-actin.

We have compared the osmotic properties of the hydrated, native actin filament and of hydrated phalloidin-F-actin. We have found that phalloidin-F-actin interacts much more strongly with water than native F-actin. It is therefore very likely that the interaction with myosin (that requires the expulsion of the protein solvation water) is more problematic for phalloidin-F-actin that for native F-actin. We conclude that phalloidin-F-actin is not a bona fide substitute for native F-actin in the "in vitro motility assay".

Actins↗

Osmotic properties of the calcium-regulated actin filament.

The diameter of the actin filament decreases with an increase of the protein osmotic pressure. This phenomenon is accompanied by a decrease of the angle (alpha) formed between the long axis of the actin monomer and the pointed end of the filament axis. At 1.8 x 10(5) dyn/cm2 (the protein osmotic pressure in frog muscle) the diameter is 8.34 nm and the angle (alpha) is 61.5 degrees. The interfilament distance of tropomyosin-decorated actin filaments, at a set of different osmotic pressures, is larger than that of F-actin filaments. This suggests that the two tropomyosin helices project out of the contour of the actin filament. The tropomyosin-decorated actin filament is more rigid than F-actin. At 1.8 x 10(5) dyn/cm2, the angle (alpha) is 76.4 degrees, as compared to the value of 61.5 degrees for F-actin. The interfilament distance of troponin-tropomyosin-decorated actin filaments is sensitive to Ca2+: in the physiological range of protein osmotic pressure it decreases from 13.3 nm, in the presence of 2 mM EGTA, to 12.2 nm in the presence of 0.2 mM CaCl2. Two alternative models are proposed to explain the decrease in interfilament distance. (a) Calcium shifts tropomyosin along the actin monomer, toward the filament axis (the classical model). (b) Calcium releases the rigidity of the tropomyosin-decorated filament and restores the original plasticity of F-actin. The consequent decrease of the angle (alpha) brings the tropomyosin helices nearer to the filament axis, without any real movement of tropomyosin along the actin monomer.

Actin Cytoskeleton↗

Actin may contribute to the power stroke in the binary actomyosin system.

At the physiological protein osmotic pressure, the angle formed between the long axis of the actin monomer and the pointed end of the filament axis is roughly 61 degrees in F-actin and about 90 degrees in the myosin subfragment 1--decorated F-actin. This implies that, in the course of the contractile cycle, actin itself contributes, by about 4 nm, to the displacement of the actin filament toward the center of the sarcomer.

Actins↗

alpha-Actinin from chicken gizzard: at low temperature, the onset of actin-gelling activity correlates with actin bundling.

The effect of alpha-actinin from chicken gizzard on the properties of F-actin solutions at 37 degrees C and at 4 degrees C was investigated. Beside the well-known increase of the gelling activity of alpha-actinin, it was found that lowering temperature to 4 degrees C: (a) modifies the shape of the alpha-actinin-F-actin binding isotherm; (b) increases the light scattering of the alpha-actinin-F-actin mixtures; (c) induces the formation of ribbons and bundles of F-actin. It was also observed that, by warming to 37 degrees C, the bundles of F-actin formed at 4 degrees C were dissociated into quasi-parallel actin filaments running at a distance of 25-42 nm from each other. On subsequent cooling to 4 degrees C, these parallel filaments were rapidly assembled into bundles. As at 37 degrees C, alpha-actinin displays a potent gelling activity on bundles but not on filaments of actin, and as the gelling activity at 4 degrees C is accompanied by the formation of actin bundles, it is concluded that actin bundling is a necessary condition to promote the actin-gelling activity.

Actinin↗

Diffusion hindrance and geometry of filament crossings account for the complex interactions of F-actin with alpha-actinin from chicken gizzard.

The interaction of alpha-actinin from chicken gizzard with F-actin is quite complex. The apparent dissociation constant, C, increases with the increase of actin concentration according to the following expression: C = Ko + a[actin] - c[actin]5/2. At pH 7.5 and 37 degrees C, in the presence of 0.1 M KCl and 2 mM MgCl2, the dissociation constant at infinite actin dilution, Ko, is 2.17 microM. The binding of alpha-actinin to actin is related by the term a[actin] to the diffusion of actin filaments and by the term c[actin]5/2 to the crossing number concentration of the F-actin network. Especially at low actin concentration, the binding of alpha-actinin to actin is increased by gelsolin, which fragments actin filaments and increases their diffusion. The different binding isotherms of alpha-actinin to actin filaments and to actin bundles are discussed.

Actinin↗

A computer-assisted automatic method for myelinated nerve fiber morphometry.

This paper describes a computer-assisted automatic method developed for myelinated nerve fiber morphometry. IBAS image analysis system was used. One-micron thick sections of sural nerve were stained with p-phenylenediamine. Dark myelin sheaths, standing out against a pale background, were identified by a binary transformation of the computer-stored image. Different parameters of the fibers as well as of the axons can be measured. The automatic system allows operator-interactive manipulation, if required, to avoid inclusion of wrong histologic structures. A large spectrum of statistics facilities are available. We performed a comparison between automatic and semi-automatic analysis. Measurements resulted virtually overlapping, but time was three to four times shorter with automatic procedure. The method here described is accurate and reliable, and permits economy of time and effort.

Biopsy↗

Binding of alpha-actinin to F-actin or to tropomyosin F-actin is a function of both alpha-actinin concentration and gel structure.

We have studied by electron microscopy as well as by measurements of low shear viscosity, rigidity and binding, the effect of alpha-actinin on the gel formed at 37 degrees C with F-actin and with tropomyosin-decorated F-actin. Contrary to previous reports in the literature, alpha-actinin at nanomolar concentrations is an efficient actin gelling protein, even at 37 degrees C, provided that the concentration of actin (or of tropomyosin-decorated F-actin) is low (1.2-2.4 microM). The binding of alpha-actinin to F-actin, as a function of actin concentration, is anomalous. The amount of bound alpha-actinin increases when actin concentration increases from 0 to 1.2 microM but does not change significantly when actin concentration is further increased up to 48 microM. A similar result is obtained with tropomyosin-decorated F-actin. These observations can be explained by an hypothesis that binding is a function of the alpha-actinin - F-actin association constant as well as of the rigidity of the gel. When the concentration of actin increases, the rigidity of the gel also increases and more work is required to bring two actin filaments to the reaction distance with alpha-actinin and, consequently, a larger alpha-actinin concentration is required to attain the same ratio of bound alpha-actinin to actin monomers in the filaments.

Actinin↗

The actin gelling activity of chicken gizzard alpha-actinin at physiological temperature is triggered by water sequestration.

At 37 degrees C, in the presence of 6% (w/v) polyethylene glycol 6000, 30 nM alpha-actinin from chicken gizzard induces the gelation of 12 microM actin. Static measurement shows that the addition of 30 nM alpha-actinin increases the rigidity of the system from 23.5 to 54 dynes/cm2. According to the theory of osmoelastic coupling, also large additives, such as the proteins of the cell sap, are able to cause an osmotic stress equivalent to that caused by polyethylene glycol. We thus conclude that, in vivo, alpha-actinin acts as an actin gelling protein.

Actinin↗

Divergent effects of filamin and tropomyosin on actin filaments bundling.

Filamin increases and tropomyosin decreases the susceptibility of F-actin to form bundles of filaments in the presence of polyethylene glycol 6000. The two proteins, which are located in the leading edge and in the internal part of the cell, respectively, are thus likely to display divergent effects on the microfilaments into bundles transition in these two areas of the cell.

Actin Cytoskeleton↗

Microfilament gel rigidity cooperates negatively with the binding of actin gelling proteins.

At 37 degrees C, in the presence of 0.1 M KC1 and 2 mM MgCl2, the binding of alpha-actinin to F-actin increases with the concentration of alpha-actinin but not with the concentration of F-actin. This implies that binding is determined by additional factors, beside the alpha-actinin - F-actin association constant. We propose that one of these factors is the rigidity of the gel, which cooperates negatively to the binding by increasing the work needed to bring two actin filaments at the reaction distance with alpha-actinin.

Actin Cytoskeleton↗

Substoichiometric concentrations of ATP-G-actin are required to anneal actin polymerized by calcium ions.

At 3 degrees C and pH 7.0, the addition of 40 nM ATP-G-actin to F-actin (12 microM as the monomer), polymerized in the presence of 4 mM CaCl2, determines a substantial and rapid increase of the viscosity of the solution, which is accompanied by the incorporation of the ATP-G-actin added into the polymer. The hypothesis that the presence of ATP-actin at the filament end(s) promotes the annealing reaction is substantiated by the finding that, after the addition of ATP-G-actin, the average filament length is increased. This finding is relevant, not only because it provides evidences in favour of the existence of annealing but also because it shows that the concentration of ATP-G-actin influences the filaments length distribution through a mechanism different from the elongation reaction.

Actins↗

Fructose bisphosphate aldolase from rabbit muscle. A jump in the van't Hoff plot accompanies the onset of half of the sites' reactivity.

In 40% ethylene glycol, gamma/2 = 0.11 and pH* 8.2, fructose 1,6-bisphosphate aldolase from rabbit muscle undergoes a transition: above 3 degrees C it displays 4 equivalent dihydroxyacetone phosphate binding sites, below -1 degree C the sites decrease to 2. The dissociation constant of the aldolase-dihydroxyacetone phosphate complex decreases from 10 microM at 3 degrees C to 2.65 microM at -1 degree C, its van't Hoff plot being linear between -1 degree C and -13 degrees C. The rate of the detritiation of the aldolase-(3S)-[3-3H]dihydroxyacetone phosphate complex is strongly influenced by temperature. In 40% ethylene glycol, gamma/2 = 0.01 and pH* 8.2, the apparent rate constant is 7.6 sec-1 at -5 degrees C and 0.012 sec-1 at -24 degrees C. The Arrhenius plot is linear between -5 degrees C and -24 degrees C.

Animals↗