Ca2+ control of actin gelation. Interaction of gelsolin with actin filaments and regulation of actin gelation

We elucidated the mechanism by which gelsolin, a Ca2+-dependent regulatory protein from lung macrophages, controls the network structure of actin filaments. In the presence of micromolar Ca2+, gelsolin bound Ca2+. The Ca2+-gelsolin complex reduced the apparent viscosity and flow birefringence of F-actin and the lengths of actin filaments viewed in the electron microscope. However, concentrations of gelsolin causing these alterations did not effect proportionate changes in the turbidity of actin filament solutions or in the quantity of nonsedimentable actin as determined by a radioassay. From these findings, we conclude that gelsolin shortens actin filaments without net depolymerization. Such an effect on the distribution of actin filament lengths led to the prediction that low concentrations of gelsolin would increase the critical concentration of actin-binding protein required for incipient gelation of actin filaments in the presence of Ca2+, providing an efficient mechanism for controlling actin network structure. We verified the prediction experimentally, and we estimated that the Ca2+-gelsolin complex effectively breaks the bond between actin monomers in filaments with a stoichiometry of 1:1. The effect of Ca2+-gelsolin complex on actin solation was rapid, independent of temperature between 0 degrees and 37 degrees C, and reversed by reducing the free Ca2+ concentration.     

The bundling of actin with polyethylene glycol 8000 in the presence and absence of gelsolin.

Actin filament and bundle formation occur in the cytosol under conditions of very high total macromolecular concentration. In this study we have utilized the inert molecule polyethylene glycol 8000 (PEG) as a means of simulating crowded conditions in vitro. Column-purified Ca-actin was polymerized in the absence and presence of gelsolin (to regulate mean filament lengths between 50 and 5000 mers) and PEG (2-8%) using various concentrations of KCl and/or 2 mM divalent cations. Bundling was characterized by the scattered light intensity and mean diffusion coefficients obtained from dynamic light scattering, as well as by fluorescence and phase-contrast microscopy. The minimum concentration of KCl required for bundling decreases both with increasing concentration of PEG at a fixed mean filament length, and with decreasing filament length at a fixed concentration of PEG. In the absence of divalent cation, bundling is reversible on dilution, as determined by intensity levels, diffusion coefficients, and microscopy. However, with either 2 mM Mg2+ or Ca2+ added, bundling is irreversible under conditions of higher PEG concentrations or longer filaments, indicating that osmotic pressure effects cannot fully explain actin bundling with PEG. Weaker divalent cation-binding sites on actin as well as disulfide bonds appear to be involved in the irreversible bundling.     

Kinetic mechanism of end-to-end annealing of actin filaments

We investigated the effect of actin filament length and capping protein on the rate of end-to-end annealing of actin filaments. Long filaments were fragmented by shearing and allowed to recover. Stabilizing filaments with phalloidin in most experiments eliminated any contribution of subunit dissociation and association to the redistribution of lengths but did not affect the results. Two different assays, fluorescence microscopy to measure filament lengths and polymerization to measure concentration of barbed filament ends, gave the same time-course of annealing. The rate of annealing declines with time as the average filament length increases. Longer filaments also anneal slower than short filaments. The second-order annealing rate constant is inversely proportional to mean polymer length with a value of 1.1 mM(-1) s(-1)/length in subunits. Capping protein slows but does not prevent annealing. Annealing is a highly favorable reaction with a strong influence on the length of polymers produced by spontaneous polymerization and should be considered in thinking about polymer dynamics in cells.     

Ca2+ regulation of gelsolin activity: binding and severing of F-actin.

Regulation of the F-actin severing activity of gelsolin by Ca2+ has been investigated under physiologic ionic conditions. Tryptophan fluorescence intensity measurements indicate that gelsolin contains at least two Ca2+ binding sites with affinities of 2.5 x 10(7) M-1 and 1.5 x 10(5) M-1. At F-actin and gelsolin concentrations in the range of those found intracellularly, gelsolin is able to bind F-actin with half-maximum binding at 0.14 microM free Ca2+ concentration. Steady-state measurements of gelsolin-induced actin depolymerization suggest that half-maximum depolymerization occurs at approximately 0.4 microM free Ca2+ concentration. Dynamic light scattering measurements of the translational diffusion coefficient for actin filaments and nucleated polymerization assays for number concentration of actin filaments both indicate that severing of F-actin occurs slowly at micromolar free Ca2+ concentrations. The data suggest that binding of Ca2+ to the gelsolin-F-actin complex is the rate-limiting step for F-actin severing by gelsolin; this Ca2+ binding event is a committed step that results in a Ca2+ ion bound at a high-affinity, EGTA-resistant site. The very high affinity of gelsolin for the barbed end of an actin filament drives the binding reaction equilibrium toward completion under conditions where the reaction rate is slow.     

Dynamic changes in the length distribution of actin filaments during polymerization can be modulated by barbed end capping proteins

During actin polymerization, it has been theorized that the actin filament length distribution initially grows in the form of a Gaussian before converting to produce that of an exponential. However, it has been difficult to demonstrate this experimentally. In this study, we use modern fluorescence microscopy techniques to observe the changing actin filament length distribution during and subsequent to the polymerization process. Nucleated actin filament growth using barbed end capping proteins (gelsolin and erythrocyte capping protein) leads to Gaussian length distributions that are relatively stable. As predicted, nucleated actin filament growth using actin/spectrin complexes follows a similar process until polymerization reaches equilibrium whereafter the Gaussian length distribution rapidly converts to that of an exponential. This study provides direct confirmation of the original theories for the mode of actin polymerization but raises doubts regarding the mechanism of the length distribution conversion from Gaussian to exponential.     

Effect of filamin and controlled linear shear on the microheterogeneity of F-actin/gelsolin gels

We have previously established [Cortese and Frieden, J. Cell Biol. 107:1477-1487, 1988] that actin gels formed under shear are microheterogeneous. In this study, the effect of cross-linking (by chicken gizzard filamin), severing (by plasma gelsolin), and shear on actin microheterogeneity are investigated using fluorescence photobleaching recovery and video microscopy. We find that filamin and shear form microheterogeneous F-actin:gelsolin gels by different mechanisms. Bundling of actin:gelsolin filaments by filamin can be explained by an increase in the apparent length of the filaments due to interfilament binding, resulting in a decrease of the polymer number concentration at which filaments organize into anisotropic phases. Some intrafilament binding of filamin to actin filaments may also be present, and those filaments coated with filamin immobilize more slowly than actin under the same polymerization conditions. The length of F-actin/gelsolin filaments seems to be a major factor in controlling the extent of bundling relative to network formation. In contrast, the effect of shear on the microheterogeneity of actin:gelsolin filaments is consistent with our previous proposal that shear aligns actin filaments, allowing filament-filament interactions and phase formation to occur. Short filaments are unable to organize into branched actin networks, but they can create large aggregates under low shear. Longer actin filaments will exist as networks with variable levels of branching and are less sensitive to shear. The effect of the intensity of a shear field on the spatial distribution of actin may involve a progressively more random orientation of actin molecules and bundles. A regular pattern develops across the sample at low shear rates (0.04-1.39 s-1), and becomes very irregular at higher shear rates (greater than 10 s-1). We suggest here that actin-binding proteins and shear can control the transition between isotropic networks and anisotropic phases by their effect on apparent length and local filament concentration, and also that this transition can have substantial effects on the resistance of cells to mechanical stress.     

Quasielastic light scattering study of thermal excitations of F-actin solutions and of growth kinetics of actin filaments.

In the first part of this work we report quasielastic light scattering (QELS) studies of the internal dynamics of transient actin networks over a time range of 10(-6)-10(-2) s, scattering angles between zeta = 20 degrees and 150 degrees, and a concentration range of 0.015 (0.3) to 0.7 mg/mL (15 microM). We confirm our previous result that (1) the dynamic structure factor g(q,t) is determined by the thermally excited undulations of the actin filaments and (2) that the initial decay of g(q, t) scales as g(q, t) varies; is directly proportional to exp(-q alpha t) while the long time decay scales as g(q, t) varies; is directly proportional to exp [-(Aq alpha t) 2/3] with alpha = 2.75. The deviation of alpha from the theoretical value of alpha = 3 predicted for Rouse-Zimm chains is similar to that found for high molecular weight macromolecular solutions by QELS. A refined analysis of the dynamic structure factor showed that it can be interpreted in terms of three relaxation processes (besides the contribution of the residual monomer diffusion): (1) the dominant Rouse-Zimm dynamics, which comprises between 65 (at high concentrations) and 85% of the signal; (2) a fast relaxation process with a decay constant of gamma = 9 x 10(3) s-1, which contributes at all concentrations with the same amplitude; and (3) a nonexponential ultraslow contribution of the form g(us) varies; is directly proportional to exp [(-gamma ust)]1/4. The third contribution appears only at high concentrations and increases strongly with decreasing scattering angles. It is thus attributed to fluctuations of the mesh size of the transient actin network. In the second part we show that high sensitivity QELS may be applied to follow the actin polymerization process at low temperatures (10 degrees C). The apparent diffusion coefficient and the static scattering intensity of the actin filaments were determined as functions of polymerization time tpol. We show that the process consists of the rapid growth of a few filaments that become very long (approximately 10 microns; even at actin concentrations of 0.04 micrograms/mL) near the critical growth concentration of 0.012 micrograms/mL, as is expected for a growth process determined by nucleation. Finally, we studied actin networks polymerized in the presence of complexes of gelsolin with actin. By application of the CONTIN program we could determine the length distribution of the filaments.(ABSTRACT TRUNCATED AT 400 WORDS)     

Tracer diffusion through F-actin: effect of filament length and cross-linking.

We have determined diffusion coefficients for small (50- to 70-nm diameter) fluorescein-thiocarbamoyl-labeled Ficoll tracers through F-actin as a function of filament length and cross-linking. fx45 was used to regulate filament length and avidin/biotinylated actin or ABP-280 was used to prepare cross-linked actin gels. We found that tracer diffusion was generally independent of filament length in agreement with theoretical predictions for diffusion through solutions of rods. However, in some experiments diffusion was slower through short (< or = 1.0 micron) filaments, although this result was not consistently reproducible. Measured diffusion coefficients through unregulated F-actin and filaments of lengths > 1.0 micron were more rapid than predicted by theory for tracer diffusion through rigid, random networks, which was consistent with some degree of actin bundling. Avidin-induced cross-linking of biotinylated F-actin did not affect diffusion through unregulated F-actin, but in cases where diffusion was slower through short filaments this cross-linking method resulted in enhanced tracer diffusion rates indistinguishable from unregulated F-actin. This finding, in conjunction with increased turbidity of 1.0-micron filaments upon avidin cross-linking, indicated that this cross-linking method induces F-actin bundling. By contrast, ABP-280 cross-linking retarded diffusion through unregulated F-actin and decreased turbidity. Tracer diffusion under these conditions was well approximated by the diffusion theory. Both cross-linking procedures resulted in gel formation as determined by falling ball viscometry. These results demonstrate that network microscopic geometry is dependent on the cross-linking method, although both methods markedly increase F-actin macroscopic viscosity.     

Polyphosphoinositide micelles and polyphosphoinositide-containing vesicles dissociate endogenous gelsolin-actin complexes and promote actin assembly from the fast-growing end of actin filaments blocked by gelsolin

The Ca2+-activated actin-binding protein gelsolin regulates actin filament length by severing preformed filaments and by binding actin monomers, stabilizing nuclei for their assembly into filaments. Gelsolin binds to phosphatidylinositol 4,5-bisphosphate (PIP2), with consequent inhibition of its filament severing activity and dissociation of EGTA-resistant complexes made with rabbit macrophage or human plasma gelsolin and rabbit muscle actin. This study provides evidence for an interaction of gelsolin with phosphatidylinositol monophosphate (PIP) as well as PIP2 and further describes their effects on gelsolin's function. Both phosphoinositides completely dissociate EGTA-insensitive rabbit macrophage cytoplasmic gelsolin-actin complexes and inhibit gelsolin's severing activity. The magnitude of inhibition depends strongly on the physical state of the phosphoinositides, being maximal in preparations that contain small micelles of either purified PIP or PIP2. Aggregation of PIP or PIP2 micelles by divalent cations or insufficient sonication or their incorporation into vesicles containing other phospholipids decreases but does not eliminate the inhibitory properties of the polyphosphoinositides. The presence of gelsolin partly inhibits the divalent cation-induced aggregation of PIP2 micelles. PIP2 in combination with EGTA inactivates gelsolin molecules that block the fast-growing end of actin filaments, thereby accelerating actin polymerization. Regulation of gelsolin by the intracellular messengers Ca2+ and polyphosphoinositides allows for the formation of several different gelsolin-actin intermediates with distinct functional properties that may be involved in changes in the state of cytoplasmic actin following cell stimulation.     

Purification and characterization of a Ca2+-dependent actin filament severing protein from bovine adrenal medulla

We describe the purification of an actin regulatory protein from bovine adrenal medulla. This protein caused a dose-dependent decrease of the specific viscosity of actin solution within 30 s of its addition in a Ca2+-sensitive way. Sedimentation assays and the observation by electron microscopy showed that this effect was ascribable to the fragmentation of actin filaments. This protein apparently promoted nucleation of actin polymerization and increased the critical concentration of actin for polymerization nearly 5-fold, suggesting its binding to the barbed end of actin filaments. The inhibitory effect of this protein on the elongation of actin from the barbed end of the myosin subfragment S1-labeled actin seeds confirmed this suggestion. These properties are similar to those of gelsolin. However, the physicochemical properties of this protein having a single polypeptide chain with a molecular weight of 74,000, a Stokes radius of 3.9 nm, a sedimentation coefficient (s0(20),w) of 4.5 S, and an immunological characterization showed that this protein is different from gelsolin.     

Kinetic analysis of F-actin depolymerization in the presence of platelet gelsolin and gelsolin-actin complexes

Platelet gelsolin (G), a 90,000-mol-wt protein, binds tightly to actin (A) and calcium at low ionic strength to form a 1:2:2 complex, GA2Ca2 (Bryan, J., and M. Kurth, 1984, J. Biol. Chem. 259:7480-7487). Chromatography of actin and gelsolin mixtures in EGTA-containing solutions isolates a stable binary complex, GA1Ca1 (Kurth, M., and J. Bryan, 1984, J. Biol. Chem. 259:7473-7479). The effects of platelet gelsolin and the binary gelsolin-actin complex on the depolymerization kinetics of rabbit skeletal muscle actin were studied by diluting pyrenyl F-actin into gelsolin or complex-containing buffers; a decrease in fluorescence represents disassembly of filaments. Dilution of F- actin to below the critical concentration required for filament assembly gave a biphasic depolymerization curve with both fast and slow components. Dilution into buffers containing gelsolin, as GCa2, increased the rate of depolymerization and gave a first order decay. The rate of decrease in fluorescence was found to be gelsolin concentration dependent. Electron microscopy of samples taken shortly after dilution into GCa2 showed a marked reduction in filament length consistent with filament severing and an increase in the number of ends. Conversely, occupancy of the EGTA-stable actin-binding site by an actin monomer eliminated the severing activity. Dilution of F-actin into the gelsolin-actin complex, either as GA1Ca1 or GA1Ca2, resulted in a decrease in the rate of depolymerization that was consistent with filament end capping. This result indicates that the EGTA-stable binding site is required and must be unoccupied for filament severing to occur. The effectiveness of gelsolin, GCa2, in causing filament depolymerization was dependent upon the ionic conditions: in KCI, actin filaments appeared to be more stable and less susceptible to gelsolin, whereas in Mg2+, actin filaments were more easily fragmented. Finally, a comparison of the number of kinetically active ends generated when filaments were diluted into gelsolin versus the number formed when gelsolin can function as a nucleation site suggests that gelsolin may sever more than once. The data are consistent with a mechanism where gelsolin, with both actin-binding sites unoccupied, can sever but not cap F-actin. Occupancy of the EGTA-stable binding site yields a gelsolin-actin complex that can no longer sever filaments, but can cap filament ends.     

Functional comparison of villin and gelsolin. Effects of Ca2+, KCl, and polyphosphoinositides

A family of homologous actin-binding proteins sever and cap actin filaments and accelerate actin filament assembly. The functions of two of these proteins, villin and gelsolin, and of their proteolytically derived actin binding domains were compared directly by measuring their effects, under various ionic conditions, on the rates and extents of polymerization of pyrene-labeled actin. In 1 mM Ca2+ and 150 mM KCl, villin and gelsolin have similar severing and polymerization-accelerating properties. Decreasing [Ca2+] to 25 microM greatly reduces severing by villin but not gelsolin. Decreasing [KCl] from 150 to 10 mM at 25 microM Ca2+ increases severing by villin, but not gelsolin, over 10-fold. The C-terminal half domains of both proteins have Ca2+-sensitive actin monomer-binding properties, but neither severs filaments nor accelerates polymerization. The N-terminal halves of villin and gelsolin contain all the filament-severing activity of the intact proteins. Severing by gelsolin's N-terminal half is Ca2+-independent, but that of villin has the same Ca2+ requirement as intact villin. The difference in Ca2+ sensitivity extends to 14-kDa N-terminal fragments which bind actin monomers and filament ends, requiring Ca2+ in the case of villin but not gelsolin. Severing of filaments by villin and its N-terminal half is shown to be inhibited by phosphatidylinositol 4,5-bisphosphate, as shown previously for gelsolin (Janmey, P.A., and Stossel, T.P. (1987) Nature 325, 362-364). The functional similarities of villin and gelsolin correlate with known structural features, and the greater functional dependence of villin on Ca2+ compared to gelsolin is traced to differences in their N-terminal domains.     

Microscopic analysis of the elastic properties of nebulin in skeletal myofibrils.

The elastic properties of nebulin were studied by measuring the elasticity of single skeletal myofibrils, from which the portion of the thin filament located at the I band had been selectively removed by treatment with plasma gelsolin under rigor conditions. In this myofibril model, a portion of each nebulin molecule at the I band was expected to be free of actin filaments and exposed. The length of the exposed portion of the nebulin molecule was controlled by performing the gelsolin treatment at various sarcomere lengths. The relation between the passive tension and extension of the exposed portion of the nebulin showed a convex curve starting from a slack length, apparently in a fashion similar to that of wool. The slack sarcomere length shifted depending on the length of the exposed portion of the nebulin, however, the relation being represented by a single master curve. The elastic modulus of nebulin was estimated to be two to three orders of magnitude smaller than that of an actin filament. Based on these results, we conclude that nebulin attaches to an actin filament in a side-by-side fashion and that it does not significantly contribute to the elastic modulus of thin filaments. The relation between the passive tension and extension of connectin (titin) was obtained for a myofibril from which thin filaments had been completely removed with gelsolin under contracting conditions; this showed a concave curve, consistent with the previous results obtained in single fibers.     

Annealing accounts for the length of actin filaments formed by spontaneous polymerization

We measured the lengths of actin filaments formed by spontaneous polymerization of highly purified actin monomers by fluorescence microscopy after labeling with rhodamine-phalloidin. The length distributions are exponential with a mean of approximately 7 microm (2600 subunits). This length is independent of the initial concentration of actin monomer, an observation inconsistent with a simple nucleation-elongation mechanism. However, with the addition of physically reasonable rates of filament annealing and fragmenting, a nucleation-elongation mechanism can reproduce the observed average length of filaments in two types of experiments: 1) filaments formed from a wide range of highly purified actin monomer concentrations, and 2) filaments formed from 24 microM actin over a range of CapZ concentrations.     

Gelsolin: calcium- and polyphosphoinositide-regulated actin-modulating protein

Receptor-mediated stimulation induces massive actin polymerization and cyto-skeletal reorganization. The activity of a potent actin-modulating protein, gelsolin, is regulated both by Ca²⁺ and polyphos-phoinositides, and it may have a pivotal role in restructuring the actin cytoskeleton in response to agonist stimulation. Structure-function analysis of gelsolin has (1) indicated that its NH₂-terminal half is primarily responsible for modulating actin filament length and polymerization; and (2) elucidated mechanisms by which Ca²⁺ and phospholipids may regulate such functions. Gelsolin is functionally and structurally similar to villin, another Ca²⁺-activated actin-severing protein found in microvilli, suggesting that gelsolin may be a prototype of this family of actin-modulating proteins. A molecular variant of gelsolin is secreted and may be involved in the clearance of actin filaments released during tissue damage. The two forms of gelsolin are encoded by a single gene, and distinct messages are derived by alternative message splicing.     

Analysis of rhodamine and fluorescein-labeled F-actin diffusion in vitro by fluorescence photobleaching recovery.

Properties of filamentous acetamidofluorescein-labeled actin and acetamidotetramethylrhodamine-labeled actin (AF and ATR-actin, respectively) were examined to resolve discrepancies in the reported translational diffusion coefficients of F-actin measured in vitro by FPR and other techniques. Using falling-ball viscometry and two independent versions of fluorescence photobleaching recovery (FPR), the present data indicate that several factors are responsible for these discrepancies. Gel filtration chromatography profoundly affects the viscosity of actin solutions and filament diffusion coefficients. ATR-actin and, to a lesser degree, AF-actin show a reduction in viscosity in proportion to the fraction labeled, presumably due to filament shortening. Actin filaments containing AF-actin or ATR-actin are susceptible to photoinduced damage, including a covalent cross-linking of actin protomers within filaments and an apparent cleavage of filaments detected by a decrease of the measured viscosity and an increase in the measured filament diffusion coefficients. Quantum yields of the two photoinduced effects are quite different. Multiple cross-links are produced relative to each photobleaching event, whereas less than 1% filament cleavage occurs. Substantial differences in the filament diffusion coefficients measured by FPR are also the result of differences in illumination geometry and sampling time. However, under controlled conditions, FPR can be used as a quantitative tool for measuring the hydrodynamic properties of actin filaments. Incremented filament shortening caused by photoinduced cleavage or incremental addition of filament capping proteins produces a continuous and approximately linear increase of filament diffusion coefficients, indicating that filaments are not associated in solution. Our results indicate that actin filaments exhibit low mobilities and it is inferred that actin filaments formed in vitro by column-purified actin, under standard conditions, are much longer than has conventionally been presumed.     

Gelsolin binds to polymeric actin at a low rate.

Association of gelsolin with actin filament subunits was investigated by the decrease of the fluorescence intensity of a 7-nitro-2-oxa-1,3-diazole (NBD) label covalently linked to gelsolin. The rate constant of this reaction was found to be 4 x 10(3) M-1 s-1. Binding of NBD-labeled gelsolin to monomeric actin proceeds at a similar low rate. The rate of association of gelsolin that was unmodified to actin filament subunits was estimated too. Unmodified gelsolin was added to a mixture of actin filaments and actin-DNase I complex. The fractions of gelsolin that bound to actin filament subunits or to actin-DNase I complex depended on the relative rates of these two competing reactions. In this way it was possible to estimate the rate constant of association of unmodified gelsolin with actin filament subunits (2 x 10(4) M-1 s-1). Thus, gelsolin associates with actin filament subunits at a rate that is considerably slower than diffusion-controlled and similar to the rate of binding of gelsolin to monomeric actin.     

Isolation and properties of two actin-binding domains in gelsolin

Gelsolin is a Ca2+-sensitive 90-kDa protein which regulates actin filament length. A molecular variant of gelsolin is present in plasma as a 93-kDa protein. Functional studies have shown that gelsolin contains two actin-binding sites which are distinct in that after Ca2+-mediated binding, removal of free Ca2+ releases actin from one site but not from the other. We have partially cleaved human plasma gelsolin with alpha-chymotrypsin and identified two distinct actin-binding domains. Peptides CT17 and CT15, which contain one of the actin-binding domains, bind to actin independently of Ca2+; peptides CT54 and CT47, which contain the other domain, bind to actin reversibly in response to changes in Ca2+ concentration. These peptides sequester actin monomers inhibiting polymerization. Unlike intact gelsolin, neither group of peptides nucleates actin assembly or forms stable filament end caps. CT17 and CT15 can however sever actin filaments. Amino acid sequence analyses place CT17 at the NH2 terminus of gelsolin and CT47 at the carboxyl-terminal two-thirds of gelsolin. Circular dichroism measurements show that Ca2+ induces an increase in the alpha-helical content of CT47. These studies provide a structural basis for understanding the interaction of gelsolin with actin and allow comparison with other Ca2+-dependent actin filament severing proteins.     

Tropomyosin and gelsolin cooperate in controlling the microfilament system

Tropomyosin has been shown to cause annealing of gelsolin-capped actin filaments. Here we show that tropomyosin is highly efficient in transforming even the smallest gelsolin-actin complexes into long actin filaments. At low concentrations of tropomyosin, the effect of tropomyosin depends on the length of the actin oligomer, and the cooperative nature of the process is a direct indication that tropomyosin induces a conformational change in the gelsolin-actin complexes, altering the structure at the actin (+) end such that capping by gelsolin is abolished. At increased concentrations of tropomyosin, heterodimers, trimers, and tetramers are converted to actin filaments. In addition, evidence is presented demonstrating that gelsolin, once removed from the (+) end of the actin, can reassociate with the newly formed tropomyosin-decorated actin filaments. Interestingly, the binding of gelsolin to the tropomyosin-actin filament complexes saturates at 2 gelsolin molecules per 14 actin and 2 tropomyosins, i.e. two gelsolins per tropomyosin-regulatory unit along the filament. These observations support the view that both tropomyosin and gelsolin are likely to have important functions in addition to those proposed earlier.