Mechanism of regulation of actin polymerization by Physarum profilin

Physarum profilin reduces the rates of nucleation and elongation of F- actin and also reduces the extent of polymerization of actin at the steady state in a concentration-dependent fashion. The apparent critical concentration for polymerization of actin is increased by the addition of profilin. These results can be explained by the idea that Physarum profilin forms a 1:1 complex with G-actin and decreases the concentration of actin available for polymerization. The dissociation constant for binding of profilin to G-actin is estimated from the kinetics of polymerization of G-actin and elongation of F-actin nuclei and from the increase of apparent critical concentration in the presence of profilin. The dissociation constants for binding of Physarum profilin to Physarum and muscle actins under physiological ionic conditions are in the ranges of 1.4-3.7 microM and 11.3-28.5 microM, respectively. When profilin is added to an F-actin solution, profilin binds to G-actin which co-exists with F-actin, and then G- actin is dissociated from F-actin to compensate for the decrease of the concentration of free G-actin and to keep it constant at the critical concentration. At the steady state, free G-actin of the critical concentration is in equilibrium not only with F-actin but also with profilin-G-actin complex. The stoichiometry of 1:1 for the formation of complex between profilin and G-actin is directly shown by means of chemical cross-linking.     

Evidence for an ATP cap at the ends of actin filaments and its regulation of the F-actin steady state

The correlation between the time courses of actin polymerization under continuous sonication and the associated ATP hydrolysis has been studied. ATP hydrolysis was not mechanistically coupled to polymerization, i.e. not necessary for polymerization, but occurred on F-actin in a subsequent monomolecular reaction. Under sonication, polymerization was complete in 10 s while hydrolysis of ATP on the polymer required 200 s. A value of 0.023 s-1 was found for the first order rate constant of ATP hydrolysis on the polymer at 25 degrees C, pH 7.8, in the presence of 0.2 mM ATP, 0.1 mM CaCl2, and 1 mM MgCl2, independent of the F-actin concentration. The conversion of ATP X F-actin to ADP X F-actin was accompanied by an increase in fluorescence of a pyrenyl probe covalently attached to actin, consistent with a 2-fold greater fluorescence for ADP X F-actin than for ATP X F-actin, with a rate constant of 0.022 s-1. In contrast, the fluorescence of F-actin labeled with 7-chloro-4-nitrobenzeno-2-oxa-1,3-diazole did not change significantly when ATP or ADP was bound. The direct consequence of the uncoupling between polymerization and ATP hydrolysis is the formation of an ATP cap at the ends of the filaments, which maintains the stability of the polymer, while most of the filament contains bound ADP. The heterogeneity of the filament with respect to ATP and ADP results in a nonlinear relationship between the rate of elongation and the concentration of G-actin with a discontinuity at the critical concentration, where the rate of growth is zero. In this respect, F-actin in ATP behaves similarly to microtubules in GTP.     

The critical concentration of actin in the presence of ATP increases with the number concentration of filaments and approaches the critical concentration of actin.ADP

F-actin at steady state in the presence of ATP partially depolymerized to a new steady state upon mechanical fragmentation. The increase in critical concentration with the number concentration of filaments has been quantitatively studied. The data can be explained by a model in which the preferred pathway for actin association-dissociation reactions at steady state in the presence of ATP involves binding of G-actin . ATP to filaments, ATP hydrolysis, and dissociation of G-actin . ADP which is then slowly converted to G-actin . ATP. As a consequence of the slow exchange of nucleotide on G-actin, the respective amounts of G-actin . ATP and G-actin . ADP coexisting with F-actin at steady state depend on the filament number concentration. G-actin coexisting with F-actin at zero number concentration of filaments would then consist of G-actin . ATP only, while the critical concentration obtained at infinite number of filaments would be that for G-actin . ADP. Values of 0.35 and 8 microM, respectively, were found for these two extreme critical concentrations for skeletal muscle actin at 20 degrees C, pH 7.8, 0.1 mM CaCl2, 1 mM MgCl2, and 0.2 mM ATP. The same value of 8 microM was directly measured for the critical concentration of G-actin . ADP polymerized in the presence of ADP and absence of ATP, and it was unaffected by fragmentation. These results have important implications for experiments in which critical concentrations are compared under conditions that change the filament number concentrations.     

Activation of heavy meromyosin adenosine triphosphatase by various states of actin.

F-actin monomer (F-monomer) is formed upon the addition of neutral salt to G-actin. Since F-monomer has a digestibility similar to that of F-actin and much lower than that of G-actin, it has been proposed that F-monomer has a conformation different from that of G-actin and similar to the conformation of the subunits in F-actin. To examine whether F-monomer will enhance the magnesium-activated myosin adenosine triphosphatase (Mg2+-ATPase) as much as F-actin, the ability of partially polymerized actin populations at equilibrium to activate the Mg2+-ATPase of heavy meromyosin was investigated. Correlations were made between ATPase activities and the polymerization state of actin as determined by measurements of viscosity and digestibility. No significant activation of the heavy meromyosin ATPase was observed under conditions where G-actin or mixtures of G-actin and F-monomer were present. As polymer formation occurred at higher actin concentrations, or with increased KCl concentrations, substantial activation characteristic of F-actin was observed. The data suggest that F-monomer may undergo a further conformational change as it forms nuclei or joins onto polymers. Alternatively, the site of actin which activates the myosin ATPase may involve the crevice between two adjacent actin subunits.     

The formation of actin oligomers studied by analytical ultracentrifugation

The small oligomers formed from Mg-G-actin under favorable conditions were studied by sedimentation velocity ultracentrifugation. The critical concentration of actin at pH 7.8 in the presence of 100 microM MgCl2 and 200 microM ATP was 12.5 +/- 2.8 microM. Under these conditions, about 15% of 7.5 microM Mg-actin was converted to oligomers of subunit size four to eight in 5 h at 20 degrees C. In 100 microM MgCl2 and no free ATP, the critical concentration was about 6.5 microM, and about 22% of 7.5 microM Mg-actin was converted to dimers in 80 min. There were no detectable higher oligomers or F-actin present in either case. As determined by the analysis of ATP hydrolysis, most, if not all, of the oligomer subunits contained ATP. When 28.5 microM actin was polymerized to steady state in 100 microM MgCl2 and 200 microM ATP, about 50% of the actin was present as F-actin, consistent with the critical concentration (approximately 12.5 microM), about 50% as oligomers as large as seven subunits, and only about 5% as monomers. When solutions containing oligomers were diluted the oligomers dissociated. Alternatively, when the MgCl2 concentration was raised to 1 mM, the solutions containing oligomers polymerized more rapidly than monomeric Mg-G-actin and to the same final steady state. These data are entirely consistent with the condensation-elongation model for helical polymerization proposed by Oosawa and Kasai (Oosawa, F., and Kasai, M. (1962) J. Mol. Biol. 4, 10-21) according to which, under certain conditions, substantial amounts of short linear and helical oligomers should be formed below the critical concentration and linear oligomers should coexist with monomers and F-actin at steady state.     

The experimental basis of some recent hypotheses on the mechanism of the polymerization of actin: a reappraisal

We have studied the effect of sonication on the fluorescence of N-(1-pyrenyl)iodoacetamide-labeled F-actin as well as of native actin-pyrenyl-actin mixed oligomers in which the subunits were covalently attached to each other by phenylenebismaleimide. In both cases the fluorescence of the solution was largely decreased by sonication. We have found that this effect is due (a) to a 20-30% decrease of the specific fluorescence of the polymers. These results question the validity of the novel mechanism for the polymerization of actin recently proposed (D. Pantaloni et al. (1984) J. Biol. Chem. 259, 6274-6283). In these studies, in fact, the implicit assumption was made that the quenching of the fluorescence of the solution under sonication was due exclusively to the conversion of F-actin into G-actin.     

Detection of conformational changes in actin by proteolytic digestion: Evidence for a new monomeric species

When KCl is added to a solution of G-actin to induce full polymerization, a decrease in the rate at which actin undergoes enzymatic proteolysis occurs. This decrease cannot be accounted for by factors affecting the enzymes employed, but rather appears to be due to a change in the conformation of G-actin. Partially polymerized actin solutions also show a reduction in digestibility which is dependent on the F-actin content, suggesting that F-actin is essentially indigestible. Moreover, low rates of digestion were also observed at sub-critical actin concentrations, where actin in the presence of 0.1 m-KCl does not polymerize. This indicates that a confomational change occurs in G-actin before the polymerization step.At sub-critical concentrations in 0.1 m-KCl, actin is in a truly monomeric state as judged by its viscosity characteristics, its inability to enhance the rate of polymerization of G-actin and its possession of ATP as the actin-bound nucleotide. These data support the existence of a new species of actin, called F-ATP-actin monomer, which has the same physical properties and the same bound nucleotide as G-actin, but digestion characteristics like F-actin. Since F-ATP-actin monomers have the same low susceptibility to proteolysis as F-ADP-actin polymers, and because both G-ATP-actin and G-ADP-actin have similar high rates of digestion, the observed change in the conformation of actin cannot be due to the phosphorylated state of the actin-bound nucleotide. Instead, the conformational change appears to be caused by the addition of KCl to G-actin.The newly-detected monomeric species is considered to be an intermediate in the polymerization process where F-ATP-actin monomers form a population of polymerizable molecules which must reach a critical concentration before nucleation and F-actin polymer formation begin.     

Dynamic light-scattering study on polymerization process of muscle actin

Globular actin (G-actin) polymerizes into a fibrous form (F-actin) under physiological salt conditions. The polymerization process of muscle actin was studied by a dynamic light-scattering method. The intensity correlation functions G2(tau) of scattered light from a G-actin solution containing 2 mM Tris-HCl (pH 8.0) and 0.1 mM ATP were analyzed by a cumulant expansion method, and the translational diffusion coefficient was determined to be D = (8.07 +/- 0.10) X 10(-7) cm2/s at 20 degrees C. This D value gave a diameter of 5.3 nm for spherical G-actin including a hydration layer. Polymerization of 1-3 mg/ml G-actin in a solution containing 10 mM Tris-HCl (pH 8.0), 0.2 mM ATP and 60 mM KCl was followed by successive measurements of G2(tau) for a data accumulation period of 60-300 s/run. The time evolution of G2(tau) was analyzed by a least-squares fitting to the field correlation function of a multiexponential form g1(tau) = sigma iAi exp(-gamma i tau) with gamma 1 greater than gamma 2 greater than 3 greater than ..., and the static scattering intensity I(t) = mean value of I as a function of time t after initiation of polymerization was decomposed as I(t) = mean value of I sigma iAi. At the early stage of polymerization, a two-exponential fit gave results indicating that component 1 came from G-actin and component 2 from F-actin growing linearly with t. At the middle stage of polymerization, a three-exponential fit gave the results that component 1 came from G-actin and possibly its small oligomers, component 2 from polymers with a number-average length Ln of about 900 nm which was independent of t, and component 3 from 'ghosts' in dynamic light scattering in a semidilute regime. Component 3 was concluded to arise from restricted motions of polymers with lengths much longer than Ln in cages formed by polymers giving component 2, and a fragmentation-elongation process of F-actin was suggested to start at the middle stage of polymerization, resulting in the size redistribution of F-actin.     

Effects of chaetoglobosin J on the G-F transformation of actin

It was shown that substoichiometric concentrations of chaetoglobosin J, one of the fungal metabolites belonging to cytochalasins, inhibited the elongation at the barbed end of an actin filament. Stoichiometric concentrations of chaetoglobosin J decreased both the rate and the extent of actin polymerization in the presence of 75 mM KCl, 0.2 mM ATP and 10 mM Tris-HCl buffer at pH 8.0 and 25 degrees C. In contrast, stoichiometric concentrations of cytochalasin D accelerated actin polymerization. Chaetoglobosin J slowly depolymerized F-actin to G-actin until an equilibrium was reached. Analyses by a number of different methods showed the increase of monomer concentration at equilibrium to depend on chaetoglobosin J concentrations. F-actin under the influence of stoichiometric concentrations of chaetoglobosin J only slightly activated the Mg2+-enhanced ATPase activity of myosin at low ionic strength. It is suggested that when the structure of the chaetoglobosin-affected actin filaments is modified, the equilibrium is shifted to the monomer side, and the interaction with myosin is weakened.     

Purification and characterization of actobindin, a new actin monomer-binding protein from Acanthamoeba castellanii

Actobindin is a new actin-binding protein isolated from Acanthamoeba castellanii. It is composed of two possibly identical polypeptide chains of approximately 13,000 daltons, as determined by sodium dodecyl sulfate polyacrylamide gel electrophoresis, and with isoelectric points of 5.9. In the native state, actobindin appears to be a dimer of about 25,000 daltons by sedimentation equilibrium analysis. It contains no tryptophan and probably no tyrosine. Actobindin reduces the concentration of F-actin at steady state and inhibits the rate of filament elongation to extents consistent with the formation of a 1:1 actobindin-G-actin complex in a reaction with a KD of about 5 microM. The available data do not eliminate the possibility of other stoichiometries for the complex, but they are not consistent with any significant interaction between actobindin and F-actin. Despite the similarities between the effects of actobindin and Acanthamoeba profilin on the polymerization of Acanthamoeba actin, the two proteins are quite distinct with different native and subunit molecular weights, different isoelectric points, and different amino acid compositions. Also, unlike profilin, actobindin binds as well to rabbit skeletal muscle G-actin and to pyrenyl-labeled G-actin as it does to unmodified Acanthamoeba G-actin.     

A simple method for the isolation of actin from myxomycete plasmodia.

A new, simple method for the isolation of actin from myxomycete plasmodia has been developed. Plasmodium myosin B was incubated at 55 degrees C for 15 min in the presence of ATP or was treated with 90% acetone. By this treatment myosin was denatured completely. Actin was then extracted with a dilute ATP and cysteine solution from the heat- or acetone-treated myosin B. The method is simple and almost pure actin was obtained in high yield. The purified G-actin polymerized to F-actin on addition of 0.1 M KCl or 2 mM MgCl2. The viscosity of the purified F-actin was 8-10 dl/g. The F-actin activated muscle myosin ATPase, and actomyosin synthesized from the F-actin and muscle myosin showed superprecipitation on addition of ATP.     

Maleimidobenzoyl-G-actin: structural properties and interaction with skeletal myosin subfragment-1

We have investigated various structural and interaction properties of maleimidobenzoyl-G-actin (MBS-actin), a new, internally cross-linked G-actin derivative that does not exhibit, at moderate protein concentration, the salt--and myosin subfragment 1 (S-1)-induced polymerizations of G-actin and reacts reversibly and covalently in solution with S-1 at or near the F-actin binding region of the heavy chain (Bettache, N., Bertrand, R., & Kassab, R. (1989) Proc. Natl. Acad. Sci. U.S.A. 86, 6028-6032). The far-ultraviolet CD spectrum and alpha-helix content of the MBS-actin were identical with those displayed by native G-actin. 45Ca2+ measurements showed the same content of tightly bound Ca2+ in MBS-actin as in G-actin and the EDTA treatment of the modified protein promoted the same red shift of the intrinsic fluorescence spectrum as observed with native G-actin. Incubation of concentrated MBS-actin solutions with 100 mM KCl + 5 mM MgCl2 led to the polymerization of the actin derivative when the critical monomer concentration reached 1.6 mg/mL, at 25 degrees C, pH 8.0. The MBS-F-actin formed activated the Mg2(+)-ATPase of S-1 to the same extent as native F-actin. The MBS-G-actin exhibited a DNase I inhibitor activity very close to that found with native G-actin and was not to be at all affected by its specific covalent conjugation to S-1.(ABSTRACT TRUNCATED AT 250 WORDS)     

Binding of human angiogenin inhibits actin polymerization

Angiogenin is a potent inducer of angiogenesis, a process of blood vessel formation. It interacts with endothelial and other cells and elicits a wide range of cellular responses including migration, proliferation, and tube formation. One important target of angiogenin is endothelial cell-surface actin and their interaction might be one of essential steps in angiogenin-induced neovascularization. Based on earlier indications that angiogenin promotes actin polymerization, we studied the binding interactions between angiogenin and actin in a wide range of conditions. We showed that at subphysiological KCl concentrations, angiogenin does not promote, but instead inhibits polymerization by sequestering G-actin. At low KCl concentrations angiogenin induces formation of unstructured aggregates, which, as shown by NMR, may be caused by angiogenin’s propensity to form oligomers. Binding of angiogenin to preformed F-actin does not cause depolymerization of actin filaments though it causes their stiffening. Binding of tropomyosin and angiogenin to F-actin is not competitive at concentrations sufficient for saturation of actin filaments. These observations suggest that angiogenin may cause changes in the cell cytoskeleton by inhibiting polymerization of G-actin and changing the physical properties of F-actin.     

Study of actin filament ends in the human red cell membrane

There is conflicting evidence concerning the state of the actin protofilaments in the membrane cytoskeleton of the human red cell. To resolve this uncertainty, we have analysed their characteristics with respect to nucleation of G-actin polymerization. The effects of cytochalasin E on the rate of elongation of the protofilaments have been measured in a medium containing 0.1 M-sodium chloride and 5 mM-magnesium chloride, using pyrene-labelled G-actin. At an initial monomer concentration far above the critical concentration for the negative ("pointed") end of F-actin, high concentrations of cytochalasin reduce the elongation rate of free F-actin by about 70%. The residual rate is presumed to correspond to the elongation rate at the negative ends. By contrast, the elongation rate on red cell ghosts or cytoskeletons falls to zero, allowing for the background of self-nucleated polymerization of the G-actin. The critical concentration of the actin in the red cell membrane has been measured after elongation of the filaments by added pyrenyl-G-actin in the same solvent. It was found to be 0.07 microM, compared with 0.11 microM under the same conditions for actin alone. This is consistent with prediction for the case of blocked negative ends on the red cell actin. The rate of elongation of actin filaments, free and in the red cell membrane cytoskeleton, has been measured as a function of the concentration of an added actin-capping protein, plasma gelsolin, with a high affinity for the positive ends. The elongation rate falls linearly with increasing gelsolin concentration until it approaches a minimum when the gelsolin has bound to all positive filament ends. The elongation rate at this point corresponds to the activity of the negative ends, and its ratio to the unperturbed polymerization rate (in the absence of capping proteins) is indistinguishable from zero in the case of ghosts, but about 1 : 4 in the case of F-actin. When ATP is replaced in the system by ADP, so that the critical concentrations at the two filament ends are equalized, the difference is equally well-marked: for F-actin, the rate at the equivalence point is about 40% of that in the absence of capping protein, whereas for ghosts the nucleated polymerization rate at the equivalence point is again zero, indicating that under these conditions the negative ends contribute little or not at all to the rate of elongation.(ABSTRACT TRUNCATED AT 400 WORDS)     

Steady-state studies of the actin-activated adenosine triphosphatase activity of myosin.

Reconstituted actomyosin (ATP phosphohydrolase, EC 3.6.1.3) (0.400 mg F-actin/mg myosin) in 10.0 muM ATP loses 96% of its specific ATPase activity when its reaction concentration is decreased from 42.0 mug/ml down to 0.700 mug/ml. The loss of specific activity at the very low enzyme concentrations is prevented by the addition of more F-actin to 17.6 mug/ml. It is concluded that at low actomyosin concentrations the complex dissociates into free myosin with a very low specific ATPase activity and free F-actin with no ATPase. The dissociation of the essential low molecular weight subunits of myosin from the heavy chains at very low actomyosin concentrations may be a contributing factor. Actomyosin has its maximum specific activity at pH 7.8-8.2. The Km for ATP is 9.4 muM, which is at least 20-fold greater than myosin's Km for ATP. The actin-activated ATPase of myosin follows hyperbolic kinetics with varying F-actin concentrations. The Km values for F-actin are 0.110 muM (4.95 mug/ml) at pH 7.4 and 0.241 muM (10.8 mug/ml) at pH 7.8. The actin-activated maximum turnover numbers for myosin are 9.3 s-1 at pH 7.4 and 11.6 s-1 at pH 7.8. The actomyosin ATPase is inhibited by KCl. This KCl inhibition is not competitive with respect to F-actin, and it is not a simple form of non-competitive inhibition.     

Adsorption of actin at the air-water interface: a monolayer study

The intrinsic surface activity of the contractile protein actin has been determined from surface tension measurements using the Wilhelmy hanging-plate method. Actin, a very soluble protein, moves from the subphase to the air-water interface to make a film. In the absence of magnesium, actin is monomeric and is known as G-actin. During the compression the monomers change their conformation or orientation at the interface and they are then pushed reversibly into the subphase upon further compression. No collapse occurs. Actin monomers in the presence of magnesium become activated; at concentrations greater than some critical value, actin polymerizes to form filaments of F-actin. The actin filaments have a higher surface activity than the actin monomers either because they are more hydrophobic or because F-actin, a rigid polymer, is much more efficient at creating excluded volume. The actin filaments then form a rigid film at the interface that collapses when the surface area is decreased. At less than the critical concentration, the actin monomers are present in the subphase in their activated form. However, their concentration increases at the interface during film compression until the critical concentration is reached. The surface pressure isotherm in this case has the characteristics of a G-actin film at the beginning of the compression and of an F-actin film at the end of the compression process.     

Conformation changes of actin during formation of filaments and paracrystals and upon interaction with DNase I, cytochalasin B, and phalloidin

Spin labels attached to rabbit muscle actin became more immobilized upon conversion of actin from the G state to the F state with 50 mM KCl. Titration of G-actin with MgCl2 produced F-actin-like EPR spectra between 2 and 5 mM-actin filaments by electron microscopy. Higher concentrations of MgCl2 produced bundles of actin and eventually paracrystals, accompanied by further immobilization of spin labels. The effects of MgCl2 and KCl were competitive: addition of MgCl2 to 50 mM could convert F-actin (50 mM KCl) to paracrystalline (P) actin; the reverse titration (0 to 200 mM KCl in the presence of 20 mM MgCl2) was less complete. Addition of DNase I to G- or F-actin gave the expected amorphous electron micrographic pattern, and the actin was not sedimentable at (400,000 x g x h). EPR showed that the actin was in the G conformation. Addition of DNase I to paracrystalline actin gave the F conformation (EPR) but the actin was "G" by electron microscopy. Phalloidin converted G-actin to F-actin, had no effect on F-actin, and converted P-actin to the F state by electron microscopy but maintained the P conformation by EPR. Cytochalasin B produced no effects observable by EPR or centrifugation but "untwisted" paracrystals into nets. Since actin retained its P conformation by EPR in two states which were morphologically not P, we conclude that the P state is a distinct conformation of the actin molecule and that actin filaments aggregate to form bundles (and eventually paracrystals) when actin monomers are able to enter the P conformation.     

54Mn2+ as a tracer of the polymerization of actin. Intermediate oligomers condense to give F-actin.

Mg2+, at submicromolar concentrations, is needed for the nucleation of actin [Maruyama (1981) J. Biol. Chem. 256, 1060-1062]. I show here that Mn2+ fulfils the same function. It binds to oligomers present in the ATP-G-actin solutions with a ratio of 2-3 Mn2+ ions per 100 actin monomers and with an association constant of 0.66 X 10(10) M-1 at pH 8.2 at 25 degrees C. The time course of the binding of Mn2+ to polymerizing actin is not affected by the initial concentration of the protein. Analysis of the distribution of the binding shows that, both in the large oligomeric species and in the polymers, 1 Mn2+ ion is bound for every 14-25 actin monomers, whereas in the smaller oligomeric species 1 Mn2+ ion is bound for every 4 actin monomers. The proposal is made that Mn2+ stabilizes actin nuclei and decreases the concentration of the monomers at the steady state. It is also proposed that, at least in some experimental conditions, the direct condensation of oligomers of intermediate length is an effective mechanism of F-actin formation.     

Some properties of Physarum actinin. A regulatory protein of actin polymerization.

A factor termed Physarum actinin was isolated and partially purified from plasmodia of a myxomycete, Physarum polycephalum. When Physarum actinin was mixed with purified Physarum or rabbit striated muscle G-actin in a weight ratio of about 1 actinin to 9 actin and then the polymerization of G-actin induced, G-actin polymerized to the ordinary F-actin on addition of 0.1 M KCl. However, it polymerized to Mg-polymer on addition of 2 mM MgCl2. The reduced viscosity (etasp/C) of the Mg-polymer was 1.2 dl/g, about one-seventh of that of the F-actin (7.4 dl/g). The sedimentation coefficient of the Mg-polymer was 22.8 S, almost the same as that of the F-actin (29.4 S). The Mg-polymer showed the specific ATPase activity of the order of 1 . 10(-3) mumol ATP/mg actin per min. It was shown that Physarum actinin copolymerized with G-actin to form Mg-polymer on addition of 2 mM MgCl2. The molecular weights of Physarum actinin were about 90 000 in salt-free or slat solutions and 43 000 in a dodecyl sulfate solution. The range of salting out with ammonium sulfate was 50--65% saturation, which was different from that of Physarum actin (15--35% saturation). Physarum actinin did not interact with Physarum myosin or muscle heavy meromyosin. When the weight ratio of actinin to actin increased, the flow birefringence of the formed Mg-polymer decreased, and it became almost zero at the weight ratio of 1 actinin to 5 actin. ATPase activity reached the maximum level (2.2 . 10(-3) mumol ATP/mg actin per min) at the same ratio. On the addition of Physarum actinin to purified Physarum F-actin which had been polymerized on addition of 2 mM MgCl2 the viscosity decreased rapidly, suggesting that the F-actin filaments were broken in the smaller fragments or that they transformed to Mg-polymers. A factor with properties similar to Physarum actinin was isolated from acetone powder of sea urchin eggs.     

Torsional motion of eosin-labeled F-actin as detected in the time-resolved anisotropy decay of the probe in the sub-millisecond time range

The internal motion of F-actin in the time range from 10(-6) to 10(-3) second has been explored by measuring the transient absorption anisotropy of eosin-labeled F-actin using laser flash photolysis. The transient absorption anisotropy of eosin-F-actin at 20 degrees C has a component that decays in the submicrosecond time scale to an anisotropy of about 0.3. This anisotropy then decays with a relaxation time of about 450 microseconds to a residual anisotropy of about 0.1 after 2 ms. When the concentration of eosin-F-actin was varied in the range from 7 to 28 microM, the transient absorption anisotropy curves obtained were almost indistinguishable from each other. These results show that the anisotropy decay arises from internal motion of eosin-F-actin. Analysis of the transient absorption anisotropy curves indicates that the internal motion detected by the decay in anisotropy is primarily a twisting of actin protomers in the F-actin helix; bending of the actin filament makes a minor contribution only to the measured decay. The torsional rigidity calculated from the transient absorption anisotropy is 0.2 X 10(-17) dyn cm2 at 20 degrees C, which is about an order of magnitude smaller than the flexural rigidity determined from previous studies. Thus, we conclude that F-actin is more flexible in twisting than in bending. The calculated root-mean-square fluctuation of the torsional angle between adjacent actin protomers in the actin helix is about 4 degrees at 20 degrees C. We also found that the torsional rigidity is approximately constant in the temperature range from 5 to approximately 35 degrees C, and that the binding of phalloidin does not appreciably affect the torsional motion of F-actin.