Polymerization of ADP-actin and ATP-actin under sonication and characteristics of the ATP-actin equilibrium polymer

Polymerization under sonication has been developed as a new method to study the rapid polymerization of actin with a large number of elongating sites. The theory proposed assumes that filaments under sonication are maintained at a constant length by the constant input of energy. The data obtained for the reversible polymerization of ADP-actin under sonication have been successfully analyzed according to the proposed model and, therefore, validate the model. The results obtained for the polymerization of ATP-actin under sonication demonstrate the involvement of ATP hydrolysis in the polymerization process. At high actin concentration, polymerization was fast enough, as compared to ATP hydrolysis on the F-actin, to obtain completion of the reversible polymerization of ATP-actin before significant hydrolysis of ATP occurred. A critical concentration of 3 microM was determined as the ratio of the dissociation and association rate constants for the interaction of ATP-actin with the ATP filament ends in 1 mM MgCl2, 0.2 mM ATP. The plot of the rate of elongation of filaments versus actin monomer concentration exhibited an upward deviation at high actin concentration that is consistent with this result. The fact that F-actin at steady state is more stable than the ATP-F-actin polymer at equilibrium suggests that the interaction between ADP-actin and ATP-actin subunits at the end of the ATP-capped filament is much stronger than the interaction between two ATP-actin subunits.     

Kinetic analysis of F-actin depolymerization in polymorphonuclear leukocyte lysates indicates that chemoattractant stimulation increases actin filament number without altering the filament length distribution

The rate of filamentous actin (F-actin) depolymerization is proportional to the number of filaments depolarizing and changes in the rate are proportional to changes in filament number. To determine the number and length of actin filaments in polymorphonuclear leukocytes and the change in filament number and length that occurs during the increase in F-actin upon chemoattractant stimulation, the time course of cellular F-actin depolymerization in lysates of control and peptide-stimulated cells was examined. F-actin was quantified by the TRITC-labeled phalloidin staining of pelletable actin. Lysis in 1.2 M KCl and 10 microM DNase I minimized the effects of F-actin binding proteins and G-actin, respectively, on the kinetics of depolymerization. To determine filament number and length from a depolymerization time course, depolymerization kinetics must be limited by the actin monomer dissociation rate. Comparison of time courses of depolymerization in the presence (pointed ends free) or absence (barbed and pointed ends free) of cytochalasin suggested depolymerization occurred from both ends of the filament and that monomer dissociation was rate limiting. Control cells had 1.7 +/- 0.4 x 10(5) filaments with an average length of 0.29 +/- 0.09 microns. Chemo-attractant stimulation for 90 s at room temperature with 0.02 microM N-formylnorleucylleucylphenylalanine caused a twofold increase in F-actin and about a two-fold increase in the total number of actin filaments to 4.0 +/- 0.5 x 10(5) filaments with an average length of 0.27 +/- 0.07 microns. In both cases, most (approximately 80%) of the filaments were quite short (less than or equal to 0.18 micron). The length distributions of actin filaments in stimulated and control cells were similar.     

Binding of phosphate to F-ADP-actin and role of F-ADP-Pi-actin in ATP-actin polymerization

Our previous work (Carlier, M.-F., and Pantaloni, D. (1986) Biochemistry 25, 7789-7792) had shown that F-ADP-Pi-actin is a major intermediate in ATP-actin polymerization, due to the slow rate of Pi release following ATP cleavage on filaments. To understand the mechanism of ATP-actin polymerization, we have prepared F-ADP-Pi-actin and characterized its kinetic parameters. 32Pi binds to F-ADP-actin with a stoichiometry of 1 mol/mol of F-actin subunit and an equilibrium dissociation constant Kpi of 1.5 mM at pH 7.0 Kpi increases with pH, indicating that the H2PO-4 species binds to F-actin. ADP-Pi-actin subunits dissociate much more slowly from filament ends than ADP-actin subunits; therefore, the stability of filaments in ATP is due to terminal ADP-Pi subunits. The slow rate of dissociation of ADP-Pi-actin also explains the decrease in critical concentration of ADP-actin in the presence of Pi reported by Rickard and Sheterline (Richard, J. E., and Sheterline, P. (1986) J. Mol. Biol. 191, 273-280). The effect of Pi on the rate of actin dissociation from filaments is much more pronounced at the barbed end than at the pointed end. Using gelsolin to block the barbed end, we have shown that the two ends are energetically different in the presence of ATP and saturating Pi, but less different than in the absence of Pi. The results are interpreted within a new model for actin polymerization. It is possible that phosphate binding to F-actin can regulate motile events in muscle and nonmuscle cells.     

Role of the DNase-I-Binding Loop in Dynamic Properties of Actin Filament

Effects of proteolytic modifications of the DNase-I-binding loop (residues 39-51) in subdomain 2 of actin on F-actin dynamics were investigated by measuring the rates of the polymer subunit exchange with the monomer pool at steady state and of ATP hydrolysis associated with it, and by determination of relative rate constants for monomer addition to and dissociation from the polymer ends. Cleavage of actin between Gly-42 and Val-43 by protease ECP32 resulted in enhancement of the turnover rate of polymer subunits by an order of magnitude or more, in contrast to less than a threefold increase produced by subtilisin cleavage between Met-47 and Gly-48. Probing the structure of the modified actins by limited digestion with trypsin revealed a correlation between the increased F-actin dynamics and a change in the conformation of subdomain 2, indicating a more open state of the filament subunits relative to intact F-actin. The cleavage with trypsin and steady-state ATPase were cooperatively inhibited by phalloidin, with half-maximal effects at phalloidin to actin molar ratio of 1:8 and full inhibition at a 1:1 ratio. The results support F-actin models in which only the N-terminal segment of loop 39-51 is involved in monomer-monomer contacts, and suggest a possibility of regulation of actin dynamics in the cell through allosteric effects on this segment of the actin polypeptide chain.     

The mechanisms of ATP hydrolysis accompanying the polymerization of Mg-actin and Ca-actin

The hydrolysis of ATP that accompanies actin polymerization occurs on the F-actin subsequent to the elongation step. For Mg-actin, the rate of ATP hydrolysis is similar to the rate of elongation at low concentrations of G-actin but increases more slowly as the G-actin concentration is increased. This behavior can be quantitatively modeled by assuming that ATP hydrolysis occurs predominantly, but not exclusively, on a single subunit of Mg-F-actin at the interface between an ATP-subunit cap and an ADP-subunit core. The rates of elongation of Ca-actin and Mg-actin are similar but the rate of ATP hydrolysis on Ca-F-actin is appreciably slower than the rate of elongation at all concentrations of Ca-G-actin. The data for Ca-actin can be modeled by assuming that ATP hydrolysis occurs essentially randomly on Ca-F-actin within a large ATP cap which can be as long as 2,000 subunits in a 10,000-subunit long filament.     

Binding of IgG containing immune complexes to human neutrophil Fc gamma RII and Fc gamma RIII induces actin polymerization by a pertussis toxin-insensitive transduction pathway.

The ability of a phagocytic stimulus, rabbit IgG anti-BSA/BSA immune complexes, to increase the F-actin content of human polymorphonuclear leukocytes was quantitated by flow cytometry following staining with nitrobenzoxadiazole-phallacidin. A significant rise in F-actin assembly was induced by addition of 5 micrograms/ml immune complex. Concentrations of immune complex of more than 200 micrograms/ml caused a maximal (approximately twofold) increase in F-actin content. After a delay of 5 s, the F-actin levels rose and reached maximum levels by 60 s after adding immune complexes. The twofold elevation in F-actin persisted for up to 60 min. Both anti-Fc gamma RII and anti-Fc gamma RIII mAb blocked immune complex stimulated actin polymerization. Exposure to pertussis toxin failed to affect the rate or extent of immune complex-induced actin polymerization. Cells incubated with immune complexes and then lysed with Triton had an increased number of sites able to nucleate actin polymerization. These findings suggest that immune complex binding to both polymorphonuclear leukocytes Fc gamma RII and Fc gamma RIII is required for actin filament assembly and that the induction of assembly occurs via transduction pathways that differ from those used by chemoattractants. As with adhesion this phagocytic stimulus induces actin assembly by a pertussis toxin insensitive pathway and produces a rise in actin filament content that persists for prolonged periods of time.     

The structural basis for the intrinsic disorder of the actin filament: the "lateral slipping" model

Three-dimensional (3-D) helical reconstructions computed from electron micrographs of negatively stained dispersed F-actin filaments invariably revealed two uninterrupted columns of mass forming the "backbone" of the double-helical filament. The contact between neighboring subunits along the thus defined two long-pitch helical strands was spatially conserved and of high mass density, while the intersubunit contact between them was of lower mass density and varied among reconstructions. In contrast, phalloidinstabilized F-actin filaments displayed higher and spatially more conserved mass density between the two long-pitch helical strands, suggesting that this bicyclic hepta-peptide toxin strengthens the intersubunit contact between the two strands. Consistent with this distinct intersubunit bonding pattern, the two long-pitch helical strands of unstabilized filaments were sometimes observed separated from each other over a distance of two to six subunits, suggesting that the intrastrand intersubunit contact is also physically stronger than the interstrand contact. The resolution of the filament reconstructions, extending to 2.5 nm axially and radially, enabled us to reproducibly "cut out" the F-actin subunit which measured 5.5 nm axially by 6.0 nm tangentially by 3.2 nm radially. The subunit is distinctly polar with a massive "base" pointing towards the "barbed" end of the filament, and a slender "tip" defining its "pointed" end (i.e., relative to the "arrowhead" pattern revealed after stoichiometric decoration of the filaments with myosin subfragment 1). Concavities running approximately parallel to the filament axis both on the inner and outer face of the subunit define a distinct cleft separating the subunit into two domains of similar size: an inner domain confined to radii less than or equal to 2.5-nm forms the uninterrupted backbone of the two long-pitch helical strands, and an outer domain placed at radii of 2-5-nm protrudes radially and thus predominantly contributes to the outer part of the massive base. Quantitative evaluation of successive crossover spacings along individual F-actin filaments revealed the deviations from the mean repeat to be compensatory, i.e., short crossovers frequently followed long ones and vice versa. The variable crossover spacings and diameter of the F-actin filament together with the local unraveling of the two long-pitch helical strands are explained in terms of varying amounts of compensatory "lateral slipping" of the two strands past each other roughly perpendicular to the filament axis. This intrinsic disorder of the actin filament may enable the actin moiety to play a more active role in actin-myosin-based force generation than merely act as a rigid passive cable as has hitherto been assumed.     

Selective neoglycosylation increases the structural stability of vicilin, the 7S storage globulin from pea seeds

The effects of glycosylation on the stability and subunit interactions of vicilin, the major storage protein in pea seeds, were investigated. Glycosylated vicilin derivatives were prepared by alkylation of lysine epsilon-amino groups with various carbohydrates. Average modification levels of 13.4 +/- 3.0, 11.1 +/- 3.6, 7.5 +/- 4.2, and 4.7 +/- 0.3 moles of carbohydrate/mol of vicilin were obtained with glucose, galactose, galacturonic acid, and lactose, respectively. Nondenaturing polyacrylamide gel electrophoresis and size-exclusion chromatography indicated that the quaternary structure and hydrodynamic radius of vicilin were not affected by glycosylation at the levels used. We have previously shown that application of hydrostatic pressure causes dissociation of vicilin subunits [C. Pedrosa and S. T. Ferreira (1994) Biochemistry 33, 4046-4055]. Analysis of pressure dissociation data allowed determination of the Gibbs free energy change (deltaG(diss)) and molar volume change (deltaV(diss)) of dissociation of vicilin subunits. For unmodified vicilin, deltaG(diss) = 18.2 kcal/mol and deltaV(diss) = -102 ml/mol. Glycosylated vicilin derivatives were significantly stabilized against subunit dissociation, with deltaG(diss) of 19.4, 19.2, 20.6, and 22.1 kcal/mol for glucose, galactose, lactose, and galacturonic acid derivatives, respectively. No changes in deltaV(diss) were found for the glucose and galactose derivatives, whereas deltaV(diss) of -128 and -135 ml/mol, respectively, were found for the lactose and galacturonic acid derivatives. The glycosylated derivatives also appeared more resistant to unfolding by guanidine hydrochloride than unmodified vicilin. Intrinsic fluorescence lifetime measurements showed that glycosylation caused a significant increase in heterogeneity of the fluorescence decay, possibly reflecting increased conformational heterogeneity of glycosylated derivatives relative to unmodified vicilin. These results indicate that the stability and subunit interactions of vicilin may be modulated by mild, selective glycosylation at low modification levels, an effect that may be of interest in the study of other oligomeric proteins.     

Thiol oxidation of actin produces dimers that enhance the elasticity of the F-actin network

Slow oxidation of sulfhydryls, forming covalently linked actin dimers and higher oligomers, accounts for increases in the shear elasticity of purified actin observed after aging. Disulfide-bonded actin dimers are incorporated into F-actin during polymerization and generate cross-links between actin filaments. The large gel strength of oxidized actin (>100 Pa for 1 mg/ml) in the absence of cross-linking proteins falls to within the theoretically predicted order of magnitude for uncross-linked actin filament networks (1 Pa) with the addition of sufficient concentrations of reducing agents such as 5 mM dithiothreitol or 10 mM beta-mercaptoethanol. As little as 1 gelsolin/1000 actin subunits also lowers the high storage modulus of oxidized actin. The effects of gelsolin may be both to increase filament number as it severs F-actin and to cover the barbed end of an actin filament, which otherwise might cross-link to the side of another filament via an actin dimer. These new findings may explain why previous studies of actin rheology report a wide range of values when purified actin is polymerized without added regulatory proteins.     

Dissociative mechanism of F-actin thermal denaturation

We have applied differential scanning calorimetry to investigate thermal unfolding of F-actin. It has been shown that the thermal stability of F-actin strongly depends on ADP concentration. The transition temperature, T(m), increases with increasing ADP concentration up to 1 mM. The T(m) value also depends on the concentration of F-actin: it increases by almost 3 degrees C as the F-actin concentration is increased from 0.5 to 2.0 mg/ml. Similar dependence of the T(m) value on protein concentration was demonstrated for F-actin stabilized by phalloidin, whereas it was much less pronounced in the presence of AlF4(-). However, T(m) was independent of protein concentration in the case of monomeric G-actin. The results suggest that at least two reversible stages precede irreversible thermal denaturation of F-actin; one of them is dissociation of ADP from actin subunits, and another is dissociation of subunits from the ends of actin filaments. The model explains why unfolding of F-actin depends on both ADP and protein concentration.     

Determination of the activation volume of PLCbeta by Gbeta gamma-subunits through the use of high hydrostatic pressure

Activation of phospholipase Cbeta (PLCbeta) by G-proteins results in increased intracellular Ca(2+) and activation of protein kinase C. We have previously found that activated PLCbeta-Gbetagamma complex can be rapidly deactivated by Galpha(GDP) subunits without dissociation, which led to the suggestion that Galpha(GDP) binds to PLCbeta-Gbeta gamma and perturbs the activating interaction without significantly affecting the PLCbeta-Gbeta gamma binding energy. Here, we have used high pressure fluorescence spectroscopy to determine the volume change associated with this interaction. Since PLCbeta and G-protein subunits associate on membrane surfaces, we worked under conditions where the membrane surface properties are not expected to change. We also determined the pressure range in which the proteins remain membrane bound: PLCbeta binding was stable throughout the 1-2000 bars range, Gbeta gamma binding was stable only at high membrane concentrations, whereas Galpha(s)(GDP) dissociated from membranes above 1 kbar. High pressure dissociated PLCbeta-Gbeta gamma with a DeltaV = 34 +/- 5 ml/mol. This same volume change is obtained for a peptide derived from Gbeta which also activates PLCbeta. In the presence of Galpha(s)(GDP), the volume change associated with PLCbeta-Gbeta gamma interaction is reduced to 25 +/- 1 ml/mol. These results suggest that activation of PLCbeta by Gbeta gamma is conferred by a small (i.e., 3-15 ml/mol) volume element.     

The actin-based nanomachine at the leading edge of migrating cells.

Two fundamental parameters of the highly dynamic, ultrathin lamellipodia of migrating fibroblasts have been determined-its thickness in living cells (176 +/- 14 nm), by standing-wave fluorescence microscopy, and its F-actin density (1580 +/- 613 microm of F-actin/microm(3)), via image-based photometry. In combination with data from previous studies, we have computed the density of growing actin filament ends at the lamellipodium margin (241 +/- 100/microm) and the maximum force (1.86 +/- 0.83 nN/microm) and pressure (10.5 +/- 4.8 kPa) obtainable via actin assembly. We have used cell deformability measurements (. J. Cell Sci. 44:187-200;. Proc. Natl. Acad. Sci. USA. 79:5327-5331) and an estimate of the force required to stall the polymerization of a single filament (. Proc. Natl. Acad. Sci. USA. 78:5613-5617;. Biophys. J. 65:316-324) to argue that actin assembly alone could drive lamellipodial extension directly.     

Effects of CapZ, an actin capping protein of muscle, on the polymerization of actin

We have studied the interaction of CapZ, a barbed-end actin capping protein from the Z line of skeletal muscle, with actin. CapZ blocks actin polymerization and depolymerization (i.e., it "caps") at the barbed end with a Kd of approximately 0.5-1 nM or less, measured by three different assays. CapZ inhibits the polymerization of ATP-actin onto filament ends with ATP subunits slightly less than onto ends with ADP subunits, and onto ends with ADP-BeF3- subunits about as much as ends with ADP subunits. No effect of CapZ is seen at the pointed end by measurements either of polymerization from acrosomal processes or of the critical concentration for polymerization at steady state. CapZ has no measureable ability to sever actin filaments in a filament dilution assay. CapZ nucleates actin polymerization at a rate proportional to the first power of the CapZ concentration and the 2.5 power of the actin concentration. No significant binding is observed between CapZ and rhodamine-labeled actin monomers by fluorescence photobleaching recovery. These new experiments are consistent with but do not distinguish between three models for nucleation proposed previously (Cooper & Pollard, 1985). As a prelude to the functional studies, the purification protocol for CapZ was refined to yield 2 mg/kg of chicken breast muscle in 1 week. The activity is stable in solution and can be lyophilized. The native molecular weight is 59,600 +/- 2000 by equilibrium ultracentrifugation, and the extinction coefficient is 1.25 mL mg-1 cm-1 by interference optics. Polymorphism of the alpha and beta subunits has been detected by isoelectric focusing and reverse-phase chromatography. CapZ contains no phosphate (less than 0.1 mol/mol).     

Actin filament capping protein from bovine brain.

An actin filament capping protein has been purified from bovine brain. The protein has a native mol. wt. of 63 kilodaltons (kd) with subunits of 36 kd and 31 kd and is globular in shape. It nucleates actin polymerization, inhibits filament elongation and filament interactions, and decreases the steady state viscosity of F-actin in substoichiometric amounts (molar ration 1:1000). In addition, the protein increases the critical concentration for actin polymerization. Neither Ca2+ nor calmodulin affects it action. All these effects can be explained by the binding of the protein to the 'barbed' end of actin filaments leading to a blockade of actin monomer addition at the preferred growing end. This is directly demonstrated by electron microscopy. Concerning the polypeptide composition, Ca2+-independence, mode, and stoichiometry of actin interaction, the protein is similar to the capping protein, previously isolated from Acanthamoeba.     

Biochemical and genetic analyses provide insight into the structural and mechanistic properties of actin filament disassembly by the Aip1p cofilin complex in Saccharomyces cerevisiae

Explication of the Aip1p/cofilin/actin filament complex may lead to a more detailed understanding of the mechanisms by which Aip1p and cofilin collaborate to rapidly disassemble filaments. We further characterized the actin-Aip1p interface through a random mutagenic screen of ACT1, identifying a novel Aip1p interaction site on actin. This finding is consistent with our current ternary complex model and offers insights into how Aip1p may disturb intersubunit contacts within an actin filament. In addition, site-directed mutagenesis aimed at interfering with salt bridge interactions at the predicted Aip1p-cofilin interface revealed hyperactive alleles of cof1 and aip1 that support the ternary complex model and suggest that conformational changes in cofilin structure may be transmitted to actin filaments, causing increased destabilization. Furthermore, these data support an active role for Aip1p in promoting actin filament turnover.     

Chromaffin cell scinderin, a novel calcium-dependent actin filament-severing protein.

Scinderin, a novel Ca2+-activated actin filament-severing protein, has been purified to homogeneity from bovine adrenal medulla using a combination of several chromatographic procedures. The protein has an apparent mol. wt of 79,600 +/- 450 daltons, three isoforms (pIs 6.0, 6.1 and 6.2) and two Ca2+ binding sites (Kd 5.85 x 10(-7) M, Bmax 0.81 mol Ca2+/mol protein and Kd 2.85 x 10(-6) M, Bmax 1.87 mol Ca2+/mol protein). Scinderin interacts with F-actin in the presence of Ca2+ and produces a decrease in the viscosity of actin gels as a result of F-actin filament severing as demonstrated by electron microscopy. Scinderin is a structurally different protein from chromaffin cell gelsolin, another actin filament-severing protein described. Scinderin and gelsolin have different mol. wts, isoelectric points, amino acid composition and yield different peptide maps after limited proteolytic digestion by either Staphylococcus V8 protease or chymotrypsin. Moreover, scinderin antibodies do not cross-react with gelsolin and gelsolin antibodies fail to recognize scinderin. Immunofluorescence with anti-scinderin demonstrated that this protein is mainly localized in the subplasmalemma region of the chromaffin cell. Immunoblotting tests with the same antibodies indicated that scinderin is also expressed in brain and anterior as well as posterior pituitary. Presence of scinderin and gelsolin, two Ca2+-dependent actin filament-severing proteins in the same tissue, suggests the possibility of synergistic functions by the two proteins in the control of cellular actin filament networks. Alternatively, the actin filament-severing activity of the two proteins might be under the control of different transduction and modulating influences.     

A new model for the interaction of dystrophin with F-actin

The F-actin binding and cross-linking properties of skeletal muscle dystrophin-glycoprotein complex were examined using high and low speed cosedimentation assays, microcapillary falling ball viscometry, and electron microscopy. Dystrophin-glycoprotein complex binding to F-actin saturated near 0.042 +/- 0.005 mol/ mol, which corresponds to one dystrophin per 24 actin monomers. Dystrophin-glycoprotein complex bound to F-actin with an average apparent Kd for dystrophin of 0.5 microM. These results demonstrate that native, full-length dystrophin in the glycoprotein complex binds F-actin with some properties similar to those measured for several members of the actin cross-linking super- family of proteins. However, we failed to observe dystrophin- glycoprotein complex-induced cross-linking of F-actin by three different methods, each positively controlled with alpha-actinin. Furthermore, high speed cosedimentation analysis of dystrophin- glycoprotein complex digested with calpain revealed a novel F-actin binding site located near the middle of the dystrophin rod domain. Recombinant dystrophin fragments corresponding to the novel actin binding site and the first 246 amino acids of dystrophin both bound F- actin but with significantly lower affinity and higher capacity than was observed with purified dystrophin-glycoprotein complex. Finally, dystrophin-glycoprotein complex was observed to significantly slow the depolymerization of F-actin, Suggesting that dystrophin may lie along side an actin filament through interaction with multiple actin monomers. These data suggest that although dystrophin is most closely related to the actin cross-linking superfamily based on sequence homology, dystrophin binds F-actin in a manner more analogous to actin side-binding proteins.     

Relationship between the flexibility and the motility of actin filaments: effects of pH

Both the sliding velocity of fluorescently labeled actin filament and its persistence length as an index of the bending flexibility of the filament were examined in the motility assay as varying the pH values of the solution for preparing actin filaments. When the pH value was varied from 5.0 to 9.0 in the solution in which actin filaments were formed from the constituent monomers, the motile performance of Mg²⁺ bound actin filaments (Mg-F-actin) was apparently suppressed compared to the case of Ca²⁺ bound ones (Ca-F-actin). The persistence length for Ca-F-actin gradually increased with the increase of the pH value while the similar length for Mg-F-actin remained rather independent of the value. The largest sliding velocity of the filament, on the other hand, obtained at the persistence length of roughly 6 μm for both cases of Mg-F-actin and Ca-F-actin.     

Biochemical characterization of the L-plastin-actin interaction shows a resemblance with that of alpha-actinin and allows a distinction to be made between the two actin-binding domains of the molecule

Actin interaction with L-plastin, a plastin/fimbrins isoform of the alpha-actinin family of molecules, is poorly characterized, from the biochemical point of view. Besides, molecular modeling of the T-isoform has recently provided a complete model of interaction with filamentous actin [Volkmann, N., DeRosier, D., Matsudaira, P., and Hanein, D. (2001) J. Cell Biol. 153, 947-956]. In this study, we report that recombinant L-plastin binds actin in a manner that strongly resembles that of the alpha-actinin-actin interface. The similitudes concern the absence of specificity toward the actin isoform and the inhibition of the binding by phosphoinositides. Furthermore, the participation of actin peptides 112-125 and 360-372 in the interface together with an inhibition of the rate of pyrenyl F-actin depolymerization is in favor of a lateral binding of the plastin isoform along the filament axis and strenghtens the similitudes in the way L-plastin and alpha-actinin bind to actin. We have also investigated the functional aspect and the putative equivalence of the two actin-binding domains of L-plastin toward actin binding. We demonstrate for the first time that the two recombinant fragments, expressed as single domains, have different affinities for actin. We further analyzed the difference using chemical cross-linking and F-actin depolymerization experiments assayed by fluorescence and high-speed centrifugation. The results clearly demonstrate that the two actin-binding domains of plastin display different modes of interaction with the actin filament. We discuss these results in light of the model of actin interaction proposed for T-plastin.