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.     

Kinetics of actin elongation and depolymerization at the pointed end

We measured the rate of elongation at the pointed filament end with increasing concentrations of G-actin [J(c) function] using villin-capped actin filaments of very small (actin/villin = 3, VA3) and relatively large size (actin/villin = 18, VA18) as nuclei for elongation. The measurements were made under physiological conditions in the presence of both Mg2+ and K+. In both cases the J(c) function was nonlinear. In contrast to the barbed filament end, however, the slope of the J(c) function sharply decreased rather than increased when the monomer concentration was lowered to concentrations near and below the critical concentration c infinity. At zero monomer concentration, depolymerization at the pointed end was very slow with a rate constant of 0.02 s-1 for VA18. When VA3 was used, the nonlinearity of the J(c) function was greatly exaggerated, and the nuclei elongated at actin concentrations below the independently measured critical concentration for the pointed end. This is consistent with and confirms our previous finding [Weber, A., Northrop, J., Bishop, M. F., Ferrone, F. A., & Mooseker, M. S. (1987) Biochemistry (preceding paper in the issue)] that at an actin-villin ratio of 3 a significant fraction of the villin is free and that a series of steady states exist between villin-actin complexes of increasing size and G-actin. The rate constant of elongation seems to increase with increasing G-actin concentrations because of increasing conversion of free villin into villin-actin oligomers during the period of the measurement of the initial elongation rate. The villin-actin oligomers have a much higher rate constant of actin binding than does free villin.(ABSTRACT TRUNCATED AT 250 WORDS)     

Measurement of rate constants for actin filament elongation in solution

This paper describes a simple method to measure the rate constants for actin filament elongation using pyrene-actin fluorescence as a measure of the polymer concentration and unlabeled actin filaments as nuclei. With careful selection of conditions, the initial rate of polymerization is directly proportional to the actin monomer concentration above the critical concentration. Plots of initial rate versus actin concentration give the critical concentration (x intercept), the association rate constant, k+ (slope), and the dissociation rate constant, k-(y intercept). By calibrating the system under conditions where the absolute values of these rate constants are known from previous electron microscopic experiments [T. D. Pollard and M. S. Mooseker (1981) J. Cell Biol. 88, 654-659; J. A. Cooper, S. B. Walker, and T. D. Pollard (1983) J. Muscle Res. Cell Motil. 4, 253-262], one can calculate the absolute values of the rate constants under other conditions as well as the length of the filaments used as a nuclei. This approach has proven useful for evaluating the effect of actin-binding proteins on the polymerization process.     

Rate constants and equilibrium constants for binding of the gelsolin-actin complex to the barbed ends of actin filaments in the presence and absence of calcium

The equilibrium constant for binding of the gelsolin-actin complex to the barbed ends of actin filaments was measured by the depolymerizing effect of the gelsolin-actin complex on actin filaments. When the gelsolin-actin complex blocks monomer consumption at the lengthening barbed ends of treadmilling actin filaments, monomers continue to be produced at the shortening pointed ends until a new steady state is reached in which monomer production at the pointed ends is balanced by monomer consumption at the uncapped barbed ends. By using this effect the equilibrium constant for binding was determined to be about 1.5 X 10(10) M-1 in excess EGTA over total calcium (experimental conditions: 1 mM MgCl2, 100 mM KCl, pH 7.5, 37 degrees C). In the presence of Ca2+ the equilibrium constant was found to be in the range of or above 10(11) M-1. The rate constant of binding of the gelsolin-actin complex to the barbed ends was measured by inhibition of elongation of actin filaments. Nucleation of new filaments by the gelsolin-actin complex towards the pointed ends was prevented by keeping the monomer concentration below the critical monomer concentration of the pointed ends where the barbed ends of treadmilling actin filaments elongate and the pointed ends shorten. The gelsolin-actin complex was found to bind fourfold faster to the barbed ends in the presence of Ca2+ (10 X 10(6) M-1 s-1) than in excess EGTA (2.5 X 10(6) M-1 s-1). Dissociation of the gelsolin-actin complex from the barbed ends can be calculated to be rather slow. In excess EGTA the rate constant of dissociation is about 1.7 X 10(-4) s-1. In the presence of Ca2+ this dissociation rate constant is in the range of or below 10(-4) s-1.     

Actin binding proteins that change extent and rate of actin monomer-polymer distribution by different mechanisms

Actin binding proteins control actin assembly and disassembly by altering the critical concentration and by changing the kinetics of polymerization. All of these control mechanisms in some way or the other make use of the energy of hydrolysis of actin-bound ATP. Capping of barbed filament ends increases the critical concentration as long as ATP hydrolysis maintains a difference in the actin monomer binding constants of the two ends. A further increase in the critical concentration on adding a second cap, tropomodulin, to the other, pointed filament end also requires ATP hydrolysis as described by the model presented here. Changes in the critical concentration are amplified into much larger changes of the monomer pool by actin sequestering proteins, provided their actin binding equilibrium constants fall within a relatively narrow range around the values for the two critical concentrations of actin. Cofilin greatly speeds up treadmilling, which requires ATP hydroysis, by increasing the rate constant of depolymerization. Profilin increases the rate of elongation at the barbed filament end, coupled to a lowering of the critical concentration, only if ATP hydrolysis makes profilin binding to the barbed end independent of its binding constant for actin monomers.     

Stoichiometry and stability of caldesmon in native thin filaments from sheep aorta smooth muscle.

Ca2(+)-regulated native thin filaments were extracted from sheep aorta smooth muscle. The caldesmon content determined by quantitative gel electrophoresis was 0.06 caldesmon molecule/actin monomer (1 caldesmon molecule per 16.3 actin monomers). Dissociation of caldesmon and tropomyosin from the thin filament and the depolymerization of actin was measured by sedimenting diluted thin filaments. Actin critical concentration was 0.05 microM at 10.1 and 0.13 at 10.05 compared with 0.5 microM for pure F-actin. Tropomyosin was tightly bound, with half-maximal dissociation at less than 0.3 microM thin filaments (actin monomer) under all conditions. Caldesmon dissociation was independent of tropomyosin and not co-operative. The concentration of thin filaments where 50% of the caldesmon was dissociated (CD50) ranged from 0.2 microM (actin monomer) at 10.03 to 8 microM at 10.16 in a 5 mM-MgCl2, pH 7.1, buffer. Mg2+, 25 mM at constant I, increased CD50 4-fold. CD50 was 4-fold greater at 10(-4) M-Ca2+ than at 10(-9) M-Ca2+. Aorta heavy meromyosin (HMM).ADP.Pi complex (2.5 microM excess over thin filaments) strongly antagonized caldesmon dissociation, but skeletal-muscle HMM.ADP.Pi did not. The behaviour of caldesmon in native thin filaments was indistinguishable from caldesmon in reconstituted synthetic thin filaments. The variability of Ca2(+)-sensitivity with conditions observed in thin filament preparations was shown to be related to dissociation of regulatory caldesmon from the thin filament.     

Effect of temperature on the mechanism of actin polymerization

The rate of the Mg2+-induced polymerization of rabbit skeletal muscle G-actin has been measured as as function of temperature at pH 8 by using various concentrations of Mg2+, Ca2+, and G-actin. A polymerization mechanism similar to that proposed at this pH [Frieden, C. (1983) Proc. Natl. Acad. Sci. U.S.A. 80, 6513-6517] was found to fit the data from 10 to 35 degrees C. From the kinetic data, no evidence for actin filament fragmentation was found at any temperature. Dimer formation is the most temperature-sensitive step, with the ratio of forward and reverse rate constants changing 4 orders of magnitude from 10 to 35 degrees C. Over this temperature change, all other ratios of forward and reverse rate constants change 7-fold or less, and the critical concentration remains nearly constant. The reversible Mg2+-induced isomerization of G-actin monomer occurs to a greater extent with increasing temperature, measured either by using N-(iodoacetyl)-N'-(5-sulfo-1-naphthyl)ethylenediamine-labeled actin or by simulation of the full-time course of the polymerization reaction. This is partially due to Mg2+ binding becoming tighter, and Ca2+ binding becoming weaker, with increasing temperature. Elongation rates from the filament-pointed end, determined by using actin nucleated by plasma gelsolin, show a temperature dependence slightly larger than that expected for a diffusion-limited reaction.     

Nonlinear increase of elongation rate of actin filaments with actin monomer concentration

The nonlinear increase of the elongation rate of actin filaments above the critical monomer concentration was investigated by nucleated polymerization of actin. Significant deviations from linearity were observed when actin was polymerized in the presence of magnesium ions. When magnesium ions were replaced by potassium or calcium ions, no deviations from linearity could be detected. The nonlinearity was analyzed by two simple assembly mechanisms. In the first model, if the ATP hydrolysis by polymeric actin is approximately as fast as the incorporation of monomers into filaments, terminal subunits of lengthening filaments are expected to carry to some extent ADP. As ADP-containing subunits dissociate from the ends of actin filaments faster than ATP-containing subunits, the rate of elongation of actin filaments would be nonlinearly correlated with the monomer concentration. In the second model (conformational change model), actin monomers and filament subunits were assumed to occur in two conformations. The association and dissociation rates of actin molecules in the two conformations were thought to be different. The equilibrium distribution between the two conformations was assumed to be different for monomers and filament subunits. The ATP hydrolysis was thought to lag behind polymerization and conformational change. As under the experimental conditions the rate of ATP hydrolysis by polymeric actin was independent of the concentration of filament ends, the observed nonlinear increase of the rate of elongation with the monomer concentration above the critical monomer concentration was unlikely to be caused by ATP hydrolysis at the terminal subunits. The conformational change model turned out to be the simplest assembly mechanism by which all available experimental data could be explained.     

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.     

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.     

Rabbit alveolar macrophages contain a Ca2+-sensitive, 41,000-dalton protein which reversibly blocks the "barbed" ends of actin filaments but does not sever them

A 41,000-dalton Ca2+-sensitive actin-modulating protein has been purified from rabbit alveolar macrophages using ion exchange and gel filtration chromatography. On sodium dodecyl-polyacrylamide gel electrophoresis, this macrophage protein migrates more rapidly than actin and fails to cross-react with polyclonal anti-actin antibody. It has a Stokes radius of 3.0 nm and an isoelectric point of 6.6. In the presence of micromolar Ca2+ this 41,000-Da protein: reduces the viscosity of polymerized actin, nucleates actin filament assembly, causes a nearly instantaneous increase in fluorescence intensity of subcritical concentrations of pyrenyl-actin (estimated KD of the pyrene actin-macrophage protein complex, 5 X 10(-8) M), increases the critical concentration of actin by 0.65 microM (molar ratios of protein/actin, 1/100-1/10), blocks actin monomer depolymerization from the "barbed" filament ends, and does not sever preformed actin filaments. The ability of this protein to block filament ends is rapidly and completely inhibited by lowering free calcium ion concentration below the micromolar range.     

Interaction of annexin VI with actin

Actin polymerization was investigated using fluorescence probe N-(1-pyrenyl)iodoacetamide, which was bound covalently to reactive sulfhydryl group, Cys-373. Labeled actin in the bulk was 0.5 to 1% of total actin concentration. Actin polymerization at concentration 12 mM was started by addition of 20 mM KCl and 2 mM MgCl2. The label fluorescence was excited at 365 nm and registered at 386 nm. Under actin polymerization the label fluorescence increased almost 10 times. Two main phases may be distinguished in the process of actin polymerization: 1) monomer activation and nucleus (trimer) formation, 2) growth of actin filaments on the nuclei. In our experimental conditions, both for pure actin and for that with added annexin VI, the 1st phase continued for about 3 min and after that the 2nd phase was perfectly approximated by exponential dependence. An analysis of the exponential curves showed that actin monomer lifetime increased from 327 s, at annexin absence, to about 373 s at 0.7 microM annexin and more. Calculation of rate constants at two ends of growing actin filament suggests that annexin VI binds with pointed ("slow") end so that at sufficient annexin concentration the filament grows only on barbed ("fast") end. Our results, together with data of other researchers showing that annexin VI binds with the inner membrane surface of smooth muscle cell through Ca2+, may indicate that, at Ca2+ entering the cell, this annexin binds actin filament pointed ends to cell surface making it ready for the act of contraction.     

Rate constants and equilibrium constants for binding of actin to the 1:1 gelsolin-actin complex.

The rate constant and equilibrium constant of association of an actin monomer with 1:1 gelsolin-actin complex isolated from chicken were measured by using fluorescently labeled actin. According to fluorescence stopped-flow experiments, the rate constant of formation of the 1:2 gelsolin-actin complex from 1:1 gelsolin-actin complex and actin was found to be about 2 x 10(7) M-1 s-1 under conditions where gelsolin binds Ca2+. The rate of dissociation of one actin molecule from the 1:2 gelsolin-actin complex was determined by exchange of actin for fluorescently labeled actin. The rate constant of dissociation was about 0.02 s-1. Thus, the equilibrium constant for association of actin with 1:1 gelsolin-actin complex can be calculated to be in the range of 10(9) M-1. The rate of dissociation of actin from 1:2 gelsolin-actin complex was independent of the Ca2+ concentration. Ca2+ affects only the rate of association of actin with 1:1 gelsolin-actin complex.     

Molecular mechanism of Ena/VASP-mediated actin-filament elongation

Ena/VASP proteins are implicated in a variety of fundamental cellular processes including axon guidance and cell migration. In vitro, they enhance elongation of actin filaments, but at rates differing in nearly an order of magnitude according to species, raising questions about the molecular determinants of rate control. Chimeras from fast and slow elongating VASP proteins were generated and their ability to promote actin polymerization and to bind G-actin was assessed. By in vitro TIRF microscopy as well as thermodynamic and kinetic analyses, we show that the velocity of VASP-mediated filament elongation depends on G-actin recruitment by the WASP homology 2 motif. Comparison of the experimentally observed elongation rates with a quantitative mathematical model moreover revealed that Ena/VASP-mediated filament elongation displays a saturation dependence on the actin monomer concentration, implying that Ena/VASP proteins, independent of species, are fully saturated with actin in vivo and generally act as potent filament elongators. Moreover, our data showed that spontaneous addition of monomers does not occur during processive VASP-mediated filament elongation on surfaces, suggesting that most filament formation in cells is actively controlled.     

Gelsolin as a calcium-regulated actin filament-capping protein.

Various concentrations of gelsolin (25-100 nM) were added to 2 microM polymerized actin. The concentrations of free calcium were adjusted to 0.05-1.5 microM by EGTA/Ca2+ buffer. Following addition of gelsolin actin depolymerization was observed that was caused by dissociation of actin subunits from the pointed ends of treadmilling actin filaments and inhibition by gelsolin of polymerization at barbed ends. The time course of depolymerization revealed an initial lag phase that was followed by slow decrease of the concentration of polymeric actin to reach the final steady state polymer and monomer concentration. The initial lag phase was pronounced at low free calcium and low gelsolin concentrations. On the basis of quantitative analysis the kinetics of depolymerization could be interpreted as capping, i.e. binding of gelsolin to the barbed ends of actin filaments and subsequent inhibition of polymerization, rather than severing. The main argument for this conclusion was that even gelsolin concentrations (100 nM) that exceed the concentration of filament ends ( approximately 2 nM), cause the filaments to depolymerize at a rate that is similar to the rate of depolymerization of the concentration of pointed ends existing before addition of gelsolin. The rate of capping is directly proportional to the free calcium concentration. These experiments demonstrate that at micromolar and submicromolar free calcium concentrations gelsolin acts as a calcium-regulated capping protein but not as an actin filament severing protein, and that the calcium binding sites of gelsolin which regulate the various functions of gelsolin (capping, severing and monomer binding), differ in their calcium affinity.     

Rate constants for the reactions of ATP- and ADP-actin with the ends of actin filaments

I measured the rate of elongation at the barbed and pointed ends of actin filaments by electron microscopy with Limulus sperm acrosomal processes as nuclei. With improvements in the mechanics of the assay, it was possible to measure growth rates from 0.05 to 280 s-1. At 22 degrees C in 1 mM MgCl2, 10 mM imidazole (pH 7), 0.2 mM ATP with 1 mM EGTA or 50 microM CaCl2 or with EGTA and 50 mM KCl, the elongation rates at both ends have a linear dependence on the ATP-actin concentration from the critical concentration to 20 microM. Consequently, over a wide range of subunit addition rates, the rate constants for association and dissociation of ATP-actin are constant. This shows that the nucleotide composition at or near the end of the growing filament is either the same over this range of growth rates or has no detectable effect on the rate constants. Under conditions where polymerization is fastest (MgCl2 + KCl + EGTA) the rate constants have these values: (table; see text) Compared with ATP-actin, ADP-actin associates slower at both ends, dissociates faster from the barbed end, but dissociates slower from the pointed end. Taking into account the events at both ends, these constants and a simple Oosawa-type model account for the complex three-phase dependence of the rate of polymerization in bulk samples on the concentration of ATP-actin monomers observed by Carlier, M.-F., D. Pantaloni, and E. D. Korn (1985, J. Biol. Chem., 260:6565-6571). These constants can also be used to predict the reactions at steady state in ATP. There will be slow subunit flux from the barbed end to the pointed end. There will also be minor fluctuations in length at the barbed end due to occasional rapid dissociation of strings of ADP subunits but the pointed end will be relatively stable.     

Profilin promotes barbed-end actin filament assembly without lowering the critical concentration

The mechanism of profilin-promoted actin polymerization has been systematically reinvestigated. Rates of barbed-end elongation onto Spectrin.4.1.Actin seeds were measured by right angle light scattering to avoid confounding effects of pyrenyl-actin, and KINSIM was used to analyze elongation progress curves. Without thymosin-beta4, both actin and Profilin.Actin (P.A) are competent in barbed-end polymerization, and kinetic simulations yielded the same bimolecular rate constant ( approximately 10 x 10(6) M(-1) s(-1)) for actin monomer or Profilin.Actin. When measured in the absence of profilin, actin assembly curves over a 0.7-4 microM thymosin-beta4 concentration range fit a simple monomer sequestering model (1 microM K(D) for Thymosin-beta4.Actin). The corresponding constant for thymosin-beta4.pyrenyl-Actin, however, was significantly higher ( approximately 9-10 microM), suggesting that the fluorophore markedly weakens binding to thymosin-beta4. With solutions of actin (2 microM) and thymosin-beta4 (2 or 4 microM), the barbed-end assembly rate rose with increasing profilin concentration (0.7-2 microM). Actin assembly in presence of thymosin-beta4 and profilin fit a simple thermodynamic energy cycle, thereby disproving an earlier claim (D. Pantaloni and M.-F. Carlier (1993) Cell 75, 1007-1014) that profilin promotes nonequilibrium filament assembly by accelerating hydrolysis of filament-bound ATP. Our findings indicate that profilin serves as a polymerization catalyst that captures actin monomers from Thymosin-beta4.Actin and ushers actin as a Profilin.Actin complex onto growing barbed filament ends.     

Effect of ATP removal and inorganic phosphate on length redistribution of sheared actin filament populations. Evidence for a mechanism of end-to-end annealing

The effect of inorganic phosphate (Pi) on the depolymerization of F-actin has been measured. Pi inhibits disassembly of pyrene-labelled F-actin at steady-state induced either by dilution, or by shearing, suggesting that Pi decreases the off rate constant, k-, for dissociation. This effect of Pi is maximal at 20 mM, unlike the effect of Pi in reducing the critical concentration at the pointed end (maximal at 2 mM). This difference in concentration dependence for the two effects is interpreted as different affinities of Pi for the barbed and pointed ends, presumably as ADP-Pi-actin species. The contribution of ATP/ADP phase changes at filament ends (i.e. "dynamic instability") to length redistribution in sheared polymer steady-state actin filament populations was determined by (1) converting ATP to ADP in the system to prevent phase changes, or (2) adding 20 mM-Pi to the system to inhibit depolymerization. The observed absence of effect of these treatments on length redistribution excludes all mechanisms which involve phase change-driven disassembly or monomer exchange at filament ends, and appears to constrain the mechanism to one of end-to-end annealing under these conditions.     

Actin assembly by lithium ions.

The ability of Li+ to promote the assembly of actin has been compared with the more common cations used in actin assembly assays, K+, Mg2+, and Ca2+. The principal assay of actin assembly utilized was fluorescence photobleaching recovery (FPR), from which it is possible to determine the fraction of actin protomers incorporated into filaments and the average diffusion coefficients of the filaments. In addition, critical concentrations of actin over a range of concentrations of all of these cations have been determined using an assay that involves sonication and dilution of assembled actin filaments containing trace amounts of pyrene-labeled actin. The results demonstrate that Li+ is a more potent promoter of actin assembly than is K+. The more rapid assembly of actin in the presence of Li+ is attributable to an increased rate of filament elongation. Filaments assembled in equivalent concentrations of Li+ or K+ have the same diffusion coefficients, and thus presumably the same average lengths. The critical concentration of actin is about three times less in the presence of Li+ than in the presence of an equal concentration of K+. Cytochalasin D accelerates the rate of Li+-promoted actin assembly and reduces slightly the total fraction of actin assembly. However, cytochalasin D causes less shortening of filaments in the presence of Li+ than in the presence of K+ or Mg2+. By the criteria of assembly kinetics and critical concentration, Li+ is much less potent as a promoter of actin assembly than either Mg2+ or Ca2+. These results are discussed in terms of the role of electrostatic forces in the actin assembly mechanism and in terms of possible relationships to therapeutic and toxicity mechanisms for Li+.     

Interaction of cytochalasin D with actin filaments in the presence of ADP and ATP

Cytochalasin D strongly inhibits the faster components in the reactions of actin filament depolymerization and elongation in the presence of 10 mM Tris-Cl-, pH 7.8, 0.2 mM dithiothreitol, 1 mM MgCl2, 0.1 mM CaCl2, and 0.2 mM ATP or ADP. Assuming an exclusive and total capping of the barbed end by the drug, the kinetic parameters derived at saturation by cytochalasin D refer to the pointed end and are 10-15-fold lower than at the barbed end. In ATP, the critical concentration increases with cytochalasin D up to 12-fold its value when both ends are free; as a result of the lowering of the free energy of nucleation by cytochalasin D, short oligomers of F-actin exist just above and below the critical concentration. Cytochalasin D interacts strongly with the barbed ends independently of the ADP-G-actin concentration (K = 0.5 nM-1). In contrast, the affinity of cytochalasin D decreases cooperatively with increasing ATP-G-actin concentration. These data are equally well accounted for by two different models: either cytochalasin D binds very poorly to ATP-capped filament ends whose proportion increases with actin concentration, or cytochalasin D binds equally well to ATP-ends and ADP-ends and also binds to actin dimers in ATP but not in ADP. A linear actin concentration dependence of the rate of growth was found at the pointed end, consistent with the virtual absence of an ATP cap at that end.