Rate of treadmilling of actin filaments in vitro

Cofilin drives rapid turnover and fluidization of entangled F-actin

The shape of most animal cells is controlled by the actin cortex, a thin network of dynamic actin filaments (F-actin) situated just beneath the plasma membrane. The cortex is held far from equilibrium by both active stresses and polymer turnover: Molecular motors drive deformations required for cell morphogenesis, while actin-filament disassembly dynamics relax stress and facilitate cortical remodeling. While many aspects of actin-cortex mechanics are well characterized, a mechanistic understanding of how nonequilibrium actin turnover contributes to stress relaxation is still lacking. To address this, we developed a reconstituted in vitro system of entangled F-actin, wherein the steady-state length and turnover rate of F-actin are controlled by the actin regulatory proteins cofilin, profilin, and formin, which sever, recycle, and assemble filaments, respectively. Cofilin-mediated severing accelerates the turnover and spatial reorganization of F-actin, without significant changes to filament length. We demonstrate that cofilin-mediated severing is a single-timescale mode of stress relaxation that tunes the low-frequency viscosity over two orders of magnitude. These findings serve as the foundation for understanding the mechanics of more physiological F-actin networks with turnover and inform an updated microscopic model of single-filament turnover. They also demonstrate that polymer activity, in the form of ATP hydrolysis on F-actin coupled to nucleotide-dependent cofilin binding, is sufficient to generate a form of active matter wherein asymmetric filament disassembly preserves filament number despite sustained severing.

Emergent mechanics of actomyosin drive punctuated contractions and shape network morphology in the cell cortex

Filamentous actin (F-actin) and non-muscle myosin II motors drive cell motility and cell shape changes that guide large scale tissue movements during embryonic morphogenesis. To gain a better understanding of the role of actomyosin in vivo, we have developed a two-dimensional (2D) computational model to study emergent phenomena of dynamic unbranched actomyosin arrays in the cell cortex. These phenomena include actomyosin punctuated contractions, or "actin asters" that form within quiescent F-actin networks. Punctuated contractions involve both formation of high intensity aster-like structures and disassembly of those same structures. Our 2D model allows us to explore the kinematics of filament polarity sorting, segregation of motors, and morphology of F-actin arrays that emerge as the model structure and biophysical properties are varied. Our model demonstrates the complex, emergent feedback between filament reorganization and motor transport that generate as well as disassemble actin asters. Since intracellular actomyosin dynamics are thought to be controlled by localization of scaffold proteins that bind F-actin or their myosin motors we also apply our 2D model to recapitulate in vitro studies that have revealed complex patterns of actomyosin that assemble from patterning filaments and motor complexes with microcontact printing. Although we use a minimal representation of filament, motor, and cross-linker biophysics, our model establishes a framework for investigating the role of other actin binding proteins, how they might alter actomyosin dynamics, and makes predictions that can be tested experimentally within live cells as well as within in vitro models.

Recent genetic and mechanical studies of embryonic development reveal a critical role for intracellular scaffolds in generating the shape of the embryo and constructing internal organs. In this paper we developed computer simulations of these scaffolds, composed of filamentous actin (F-actin), a rod-like protein polymer, and mini-thick filaments, composed of non-muscle myosin II, forming a two headed spring-like complex of motor proteins that can walk on, and remodel F-actin networks. Using simulations of these dynamic interactions, we can carry out virtual experiments where we change the physics and chemistry of F-actin polymers, their associated myosin motors, and cross-linkers and observe the changes in scaffolds that emerge. For example, by modulating the motor stiffness of the myosin motors in our model we can observe the formation or loss of large aster-like structures. Such fine-grained control over the physical properties of motors or filaments within simulations are not currently possible with biological experiments, even where mutant proteins or small molecule inhibitors can be targeted to specific sites on filaments or motors. Our approach reflects a growing adoption of simulation methods to investigate microscopic features that shape actomyosin arrays and the mesoscale effects of molecular scale processes. We expect predictions from these models will drive more refined experimental approaches to expose the many roles of actomyosin in development.

Covalent and non-covalent chemical engineering of actin for biotechnological applications

The cytoskeletal filaments are self-assembled protein polymers with 8-25nm diameters and up to several tens of micrometres length. They have a range of pivotal roles in eukaryotic cells, including transportation of intracellular cargoes (primarily microtubules with dynein and kinesin motors) and cell motility (primarily actin and myosin) where muscle contraction is one example. For two decades, the cytoskeletal filaments and their associated motor systems have been explored for nanotechnological applications including miniaturized sensor systems and lab-on-a-chip devices. Several developments have also revolved around possible exploitation of the filaments alone without their motor partners. Efforts to use the cytoskeletal filaments for applications often require chemical or genetic engineering of the filaments such as specific conjugation with fluorophores, antibodies, oligonucleotides or various macromolecular complexes e.g. nanoparticles. Similar conjugation methods are also instrumental for a range of fundamental biophysical studies. Here we review methods for non-covalent and covalent chemical modifications of actin filaments with focus on critical advantages and challenges of different methods as well as critical steps in the conjugation procedures. We also review potential uses of the engineered actin filaments in nanotechnological applications and in some key fundamental studies of actin and myosin function. Finally, we consider possible future lines of investigation that may be addressed by applying chemical conjugation of actin in new ways.

Kinetic Insights into the Elongation Reaction of Actin Filaments as a Function of Temperature, Pressure, and Macromolecular Crowding

Actin polymerization is an essential process in eukaryotic cells that provides a driving force for motility and mechanical resistance for cell shape. By using preformed gelsolin-actin nuclei and applying stopped-flow methodology, we quantitatively studied the elongation kinetics of actin filaments as a function of temperature and pressure in the presence of synthetic and protein crowding agents. We show that the association of actin monomers to the pointed end of double-stranded helical actin filaments (F-actin) proceeds via a transition state that requires an activation energy of 56 kJ mol(-1) for conformational and hydration rearrangements, but exhibits a negligible activation volume, pointing to a compact transition state that is devoid of packing defects. Macromolecular crowding causes acceleration of the F-actin elongation rate and counteracts the deteriorating effect of pressure. The results shed new light on the combined effect of these parameters on the polymerization process of actin, and help us understand the temperature and pressure sensitivity of actin polymerization under extreme conditions.

Bacterial actin MreB forms antiparallel double filaments

Filaments of all actin-like proteins known to date are assembled from pairs of protofilaments that are arranged in a parallel fashion, generating polarity. In this study, we show that the prokaryotic actin homologue MreB forms pairs of protofilaments that adopt an antiparallel arrangement in vitro and in vivo. We provide an atomic view of antiparallel protofilaments of Caulobacter MreB as apparent from crystal structures. We show that a protofilament doublet is essential for MreB's function in cell shape maintenance and demonstrate by in vivo site-specific cross-linking the antiparallel orientation of MreB protofilaments in E. coli. 3D cryo-EM shows that pairs of protofilaments of Caulobacter MreB tightly bind to membranes. Crystal structures of different nucleotide and polymerisation states of Caulobacter MreB reveal conserved conformational changes accompanying antiparallel filament formation. Finally, the antimicrobial agents A22/MP265 are shown to bind close to the bound nucleotide of MreB, presumably preventing nucleotide hydrolysis and destabilising double protofilaments.DOI: http://dx.doi.org/10.7554/eLife.02634.001.

Proteomic approaches to understanding the role of the cytoskeleton in host-defense mechanisms

The cytoskeleton is a cellular scaffolding system whose functions include maintenance of cellular shape, enabling cellular migration, division, intracellular transport, signaling and membrane organization. In addition, in immune cells, the cytoskeleton is essential for phagocytosis. Following the advances in proteomics technology over the past two decades, cytoskeleton proteome analysis in resting and activated immune cells has emerged as a possible powerful approach to expand our understanding of cytoskeletal composition and function. However, so far there have only been a handful of studies of the cytoskeleton proteome in immune cells. This article considers promising proteomics strategies that could augment our understanding of the role of the cytoskeleton in host-defense mechanisms.

Structural basis for the slow dynamics of the actin filament pointed end

The actin filament has clear polarity where one end, the pointed end, has a much slower polymerization and depolymerization rate than the other end, the barbed end. This intrinsic difference of the ends significantly affects all actin dynamics in the cell, which has central roles in a wide spectrum of cellular functions. The detailed mechanism underlying this difference has remained elusive, because high-resolution structures of the filament ends have not been available. Here, we present the structure of the actin filament pointed end obtained using a single particle analysis of cryo-electron micrographs. We determined that the terminal pointed end subunit is tilted towards the penultimate subunit, allowing specific and extra loop-to-loop inter-strand contacts between the two end subunits, which is not possible in other parts of the filament. These specific contacts prevent the end subunit from dissociating. For elongation, the loop-to-loop contacts also inhibit the incorporation of another actin monomer at the pointed end. These observations are likely to account for the less dynamic pointed end.

Concerning the dynamic instability of actin homolog ParM

Using in vitro TIRF- and electron-microscopy, we reinvestigated the dynamics of native ParM, a prokaryotic DNA segregation protein and actin homolog. In contrast to a previous study, which used a cysteine ParM mutant, we find that the polymerization process of wild type ATP-ParM filaments consists of a polymerization phase and a subsequent steady state phase, which is dynamically unstable, like that of microtubules. We find that the apparent bidirectional polymerization of ParM, is not due to the intrinsic nature of this filament, but results from ParM forming randomly oriented bundles in the presence of crowding agents. Our results imply, that in the bacterium, ParM filaments spontaneously form bipolar bundles. Due to their intrinsic dynamic instability, ParM bundles can efficiently "search" the cytoplasmic lumen for DNA, bind it equally well at the bipolar ends and segregate it approximately symmetrically, by the insertion of ParM subunits at either end.

Single molecules of the bacterial actin MreB undergo directed treadmilling motion in Caulobacter crescentus

The actin cytoskeleton represents a key regulator of multiple essential cellular functions in both eukaryotes and prokaryotes. In eukaryotes, these functions depend on the orchestrated dynamics of actin filament assembly and disassembly. However, the dynamics of the bacterial actin homolog MreB have yet to be examined in vivo. In this study, we observed the motion of single fluorescent MreB-yellow fluorescent protein fusions in living Caulobacter cells in a background of unlabeled MreB. With time-lapse imaging, polymerized MreB [filamentous MreB (fMreB)] and unpolymerized MreB [globular MreB (gMreB)] monomers could be distinguished: gMreB showed fast motion that was characteristic of Brownian diffusion, whereas the labeled molecules in fMreB displayed slow, directed motion. This directional movement of labeled MreB in the growing polymer provides an indication that, like actin, MreB monomers treadmill through MreB filaments by preferential polymerization at one filament end and depolymerization at the other filament end. From these data, we extract several characteristics of single MreB filaments, including that they are, on average, much shorter than the cell length and that the direction of their polarized assembly seems to be independent of the overall cellular polarity. Thus, MreB, like actin, exhibits treadmilling behavior in vivo, and the long MreB structures that have been visualized in multiple bacterial species seem to represent bundles of short filaments that lack a uniform global polarity.

Myosin-XVa is required for tip localization of whirlin and differential elongation of hair-cell stereocilia

Stereocilia are microvilli-derived mechanosensory organelles that are arranged in rows of graded heights on the apical surface of inner-ear hair cells. The 'staircase'-like architecture of stereocilia bundles is necessary to detect sound and head movement, and is achieved through differential elongation of the actin core of each stereocilium to a predetermined length. Abnormally short stereocilia bundles that have a diminished staircase are characteristic of the shaker 2 (Myo15a(sh2)) and whirler (Whrn(wi)) strains of deaf mice. We show that myosin-XVa is a motor protein that, in vivo, interacts with the third PDZ domain of whirlin through its carboxy-terminal PDZ-ligand. Myosin-XVa then delivers whirlin to the tips of stereocilia. Moreover, if green fluorescent protein (GFP)-Myo15a is transfected into hair cells of Myo15a(sh2) mice, the wild-type pattern of hair bundles is restored by recruitment of endogenous whirlin to the tips of stereocilia. The interaction of myosin-XVa and whirlin is therefore a key event in hair-bundle morphogenesis.

Crawling toward a unified model of cell mobility: spatial and temporal regulation of actin dynamics

Crawling cells of various morphologies displace themselves in their biological environments by a similar overall mechanism of protrusion through actin assembly at the front coordinated with retraction at the rear. Different cell types organize very distinct protruding structures, yet they do so through conserved biochemical mechanisms to regulate actin polymerization dynamics and vary the mechanical properties of these structures. The moving cell must spatially and temporally regulate the biochemical interactions of its protein components to exert control over higher-order dynamic structures created by these proteins and global cellular responses four or more orders of magnitude larger in scale and longer in time than the individual protein-protein interactions that comprise them. To fulfill its biological role, a cell globally responds with high sensitivity to a local perturbation or signal and coordinates its many intracellular actin-based functional structures with the physical environment it experiences to produce directed movement. This review attempts to codify some unifying principles for cell motility that span organizational scales from single protein polymer filaments to whole crawling cells.

A new ATP-binding fold in actin, hexokinase and Hsc70

One of a cell biologist's favourite occupations is to discover the proteins that perform newly described functions in the cell. Very often lately, this has resulted in the identification of protein families whose related amino acid sequences reflect similar functions, but can proteins with totally unrelated sequences have similar structures and functions? In this review, Ken Holmes, Chris Sander and Alfonso Valencia describe the structural similarities between three well-known proteins that have no readily detectable primary sequence similarities but for which X-ray crystallography has revealed very similar structures. A comparison of their structures provides insights into their common mechanisms of action and into protein evolution, and has been used to detect related proteins in sequence data bases.

Actin binding proteins: regulation of cytoskeletal microfilaments

The actin cytoskeleton is a complex structure that performs a wide range of cellular functions. In 2001, significant advances were made to our understanding of the structure and function of actin monomers. Many of these are likely to help us understand and distinguish between the structural models of actin microfilaments. In particular, 1) the structure of actin was resolved from crystals in the absence of cocrystallized actin binding proteins (ABPs), 2) the prokaryotic ancestral gene of actin was crystallized and its function as a bacterial cytoskeleton was revealed, and 3) the structure of the Arp2/3 complex was described for the first time. In this review we selected several ABPs (ADF/cofilin, profilin, gelsolin, thymosin beta4, DNase I, CapZ, tropomodulin, and Arp2/3) that regulate actin-driven assembly, i.e., movement that is independent of motor proteins. They were chosen because 1) they represent a family of related proteins, 2) they are widely distributed in nature, 3) an atomic structure (or at least a plausible model) is available for each of them, and 4) each is expressed in significant quantities in cells. These ABPs perform the following cellular functions: 1) they maintain the population of unassembled but assembly-ready actin monomers (profilin), 2) they regulate the state of polymerization of filaments (ADF/cofilin, profilin), 3) they bind to and block the growing ends of actin filaments (gelsolin), 4) they nucleate actin assembly (gelsolin, Arp2/3, cofilin), 5) they sever actin filaments (gelsolin, ADF/cofilin), 6) they bind to the sides of actin filaments (gelsolin, Arp2/3), and 7) they cross-link actin filaments (Arp2/3). Some of these ABPs are essential, whereas others may form regulatory ternary complexes. Some play crucial roles in human disorders, and for all of them, there are good reasons why investigations into their structures and functions should continue.

Transmembrane crosstalk between the extracellular matrix--cytoskeleton crosstalk

Integrin-mediated cell adhesions provide dynamic, bidirectional links between the extracellular matrix and the cytoskeleton. Besides having central roles in cell migration and morphogenesis, focal adhesions and related structures convey information across the cell membrane, to regulate extracellular-matrix assembly, cell proliferation, differentiation, and death. This review describes integrin functions, mechanosensors, molecular switches and signal-transduction pathways activated and integrated by adhesion, with a unifying theme being the importance of local physical forces.

Conformational and dynamic differences between actin filaments polymerized from ATP- or ADP-actin monomers

Conformational and dynamic properties of actin filaments polymerized from ATP- or ADP-actin monomers were compared by using fluorescence spectroscopic methods. The fluorescence intensity of IAEDANS attached to the Cys(374) residue of actin was smaller in filaments from ADP-actin than in filaments from ATP-actin monomers, which reflected a nucleotide-induced conformational difference in subdomain 1 of the monomer. Radial coordinate calculations revealed that this conformational difference did not modify the distance of Cys(374) from the longitudinal filament axis. Temperature-dependent fluorescence resonance energy transfer measurements between donor and acceptor molecules on Cys(374) of neighboring actin protomers revealed that the inter-monomer flexibility of filaments assembled from ADP-actin monomers were substantially greater than the one of filaments from ATP-actin monomers. Flexibility was reduced by phalloidin in both types of filaments.

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.

Conformational distributions and proximity relationships in the rigor complex of actin and myosin subfragment-1

Cyclic conformational changes in the myosin head are considered essential for muscle contraction. We hereby show that the extension of the fluorescence resonance energy transfer method described originally by Taylor et al. (Taylor, D. L., Reidler, J., Spudich, J. A., and Stryer, L. (1981) J. Cell Biol. 89, 362-367) allows determination of the position of a labeled point outside the actin filament in supramolecular complexes and also characterization of the conformational heterogeneity of an actin-binding protein while considering donor-acceptor distance distributions. Using this method we analyzed proximity relationships between two labeled points of S1 and the actin filament in the acto-S1 rigor complex. The donor (N-[[(iodoacetyl)amino]ethyl]-5-naphthylamine-1-sulfonate) was attached to either the catalytic domain (Cys-707) or the essential light chain (Cys-177) of S1, whereas the acceptor (5-(iodoacetamido)fluorescein) was attached to the actin filament (Cys-374). In contrast to the narrow positional distribution (assumed as being Gaussian) of Cys-707 (5 +/- 3 A), the positional distribution of Cys-177 was found to be broad (102 +/- 4 A). Such a broad positional distribution of the label on the essential light chain of S1 may be important in accommodating the helically arranged acto-myosin binding relative to the filament axis.

The rate of annealing of actin tropomyosin filaments depends strongly on the length of the filaments

Actin tropomyosin filaments were sheared to produce short filaments. Following incubation for 0 to 10000 s annealing of the filaments was assayed by determination of the rate of polymerization of monomeric actin onto the filament ends. The rate of decrease of the concentration of filament ends was found to be proportional to its fourth power. In contrast, the rate of end-to-end association of actin filaments in the absence of tropomyosin was proportional to the square of the concentration of filament ends. The strong dependence on the filament length of the rate of annealing of actin tropomyosin filaments was interpreted by the model of Hill (Biophys. J., 44, 285-288 (1983)) who pointed out that the rate constant of end-to-end association of long rod-like filaments is expected to depend on the length of the filaments for sterical conditions.

The end of a polymerizing actin filament contains numerous ATP-subunit segments that are disconnected by ADP-subunits resulting from ATP hydrolysis

ATP hydrolysis by copolymers of ATP-actin and ADP-actin was investigated in order to analyze the effect of interfaces between ATP-subunits and ADP-subunits on hydrolysis of actin-bound ATP. Copolymers of ATP- and ADP-subunits were formed by polymerization of ATP- and ADP-actin monomers onto filaments. By changing the ratio of polymerizing ATP-actin monomers to ADP-actin monomers, the number of interfaces between ATP- and ADP-subunits and of ATP-subunits only surrounded by further ATP-subunits was varied. The rate of actin polymerization and of ATP hydrolysis was measured simultaneously on the same samples. The lag time between incorporation of actin monomers into filaments and subsequent ATP hydrolysis was found to be similar both for polymerized ATP-actin and for copolymers formed by various ratios of ATP- to ADP-actin. The experiments were performed in the presence of 1 mM MgCl2, 0.05 mM CaCl2, and 100 mM KCl or of 1 mM MgCl2, and 0.4 mM EGTA. The type of cations was found to have no major effect on the rate of ATP hydrolysis. A quantitative evaluation of the experimental data suggests that ATP at interfaces between ATP- and ADP-subunits is hydrolyzed not more than 10 times faster than ATP of subunits surrounded by further ATP-subunits. On the basis of these results, one can conclude that an actin filament onto which ATP-actin monoMers polymerize contains numerous segments of ATP-subunits that are disconnected by ADP-subunits resulting from ATP hydrolysis. The average length of the numerous ATP segments of a steadily polymerizing filament is in the range of 10 ATP-subunits or below.

Two low-affinity Ca(2+)-binding sites of gelsolin that regulate association with actin

The time course of binding of actin to gelsolin or 1:1 gelsolin-actin complex was measured at defined Ca2+ concentrations in the range 0.5-500 microM. The rate of association was followed by the fluorescence increase of a fluorescent label covalently linked to actin. Free Ca2+ was determined by titration with EGTA in the presence of Fura-2 as indicator. The experimental data were quantitatively evaluated by calculations of the kinetics of association of actin with gelsolin thereby taking into account the equilibrium of binding of Ca2+ ions to gelsolin. It was found that association of gelsolin with one actin monomer is regulated by a Ca(2+)-binding site with a dissociation constant Kd1 = 25 microM. Binding of the second actin monomer was found to be controlled by a Ca(2+)-binding site of which the dissociation constant Kd2 was 200 microM. Mg2+ ions in the concentration range 0-1 mM did not compete with Ca2+ for binding to gelsolin. More complex interactions of gelsolin with actin such as nucleated actin polymerization were found to occur even at Ca2+ concentrations below Kd1 (e.g. 10 microM) at almost maximal rates.

Mechanism of ATP hydrolysis by polymeric actin

The lag between polymerization of actin and ATP hydrolysis in actin filaments was analyzed in terms of the mechanism of the hydrolysis reaction. Under the experimental conditions (100 mM KCl and 1 mM MgCl2, or without KCl, 1 mM MgCl2 and 0.4 mM EGTA, 25 degrees C) ATP hydrolysis lagged behind polymerization by about 100 s independently of the concentration of polymerizing filament ends and of the actin monomer concentration. Three models of ATP hydrolysis were compared to experimental data: (i) Random ATP hydrolysis, ATP is assumed to be hydrolyzed at a rate that is independent of the type of the nucleotide bound to adjacent filament subunits. (ii) Cooperative hydrolysis, the rate of ATP hydrolysis is thought to depend on the type of nucleotide bound to adjacent subunits. (iii) Sequential hydrolysis, ATP is assumed to be hydrolyzed only at the interface between ATP-subunits and ADP-subunits. The model of sequential ATP hydrolysis could be excluded. The results were in agreement with random or cooperative ATP hydrolysis. The differences of the rates of ATP hydrolysis by a random or cooperative mechanism are so small that based on the experimental results no distinction between these two mechanisms could be made. All available evidence points towards a mechanism of ATP hydrolysis in which several or perhaps many interfaces between ATP- and ADP-subunits are formed within a filament.

Clostridial ADP-ribosylating toxins: effects on ATP and GTP-binding proteins

The actin cytoskeleton appears to be as the cellular target of various clostridial ADP-ribosyltransferases which have been described during recent years. Clostridium botulinum C2 toxin, Clostridium perfringens iota toxin and Clostridium spiroforme toxin ADP-ribosylate actin monomers and inhibit actin polymerization. Clostridium botulinum exoenzyme C3 and Clostridium limosum exoenzyme ADP-ribosylate the low-molecular-mass GTP-binding proteins of the Rho family, which participate in the regulation of the actin cytoskeleton. ADP-ribosylation inactivates the regulatory Rho proteins and disturbs the organization of the actin cytoskeleton.

Nucleation of actin polymerization by gelsolin

The time-course of assembly of actin with gelsolin was measured by the fluorescence increase of a fluorescent label covalently linked to actin. The actin concentrations ranged from values far below the critical concentration to values above the critical concentration of the pointed ends of actin filaments. If the concentration of actin was in the range of the critical monomer concentration (0.64 microM), the time-course of the concentration of actin assembled with gelsolin revealed a sigmoidal shape. At higher actin concentrations the time-course of association of actin with gelsolin approximated an exponential curve. The measured time-courses of assembly were quantitatively interpreted by kinetic rate equations. A poor fit was obtained if two actin molecules were assumed to bind to gelsolin to form a 1:2 gelsolin-actin complex and subsequently further actin molecules were assumed to polymerize onto the 1:2 gelsolin-actin complex toward the pointed end. A considerably better agreement between calculated and measured time-courses was achieved if additional creation of actin filaments by fast fragmentation of newly formed actin filaments by not yet consumed gelsolin was assumed to occur. This suggests that both polymerization of actin onto gelsolin and fragmentation of actin filaments contribute to formation of new actin filaments by gelsolin. Furthermore it could be demonstrated that below the critical monomer concentration appreciable amounts of actin are incorporated into gelsolin-actin oligomers.

Mechanisms of the cytopathic action of actin-ADP-ribosylating toxins

Clostridium botulinum C2 toxin, Clostridium perfringens iota toxin, and Clostridium spiroforme toxin ADP-ribosylate actin monomers. Toxin-induced ADP-ribosylation disturbs the cellular equilibrium between monomeric and polymeric actin and traps monomeric actin in its unpolymerized form, thereby depolymerizing actin filaments and destroying the microfilament network. Furthermore, the toxins ADP-ribosylate gelsolin actin complexes. These modifications may contribute to the cytopathic action of the toxins.

ASP-56, a new actin sequestering protein from pig platelets with homology to CAP, an adenylate cyclase-associated protein from yeast

A new 56 kDa actin-binding protein (ASP-56) was isolated from pig platelet lysate. In falling ball viscosimetry it caused a reduction in viscosity that could be attributed to a decrease in the concentration of polymeric actin. Fluorescence measurements with NBD-labelled actin showed reduction of polymeric actin, too. These results could be explained by sequestering of actin in a non-polymerizable 1:1 ASP-56/actin complex. Sequencing of about 20 tryptic peptides of ASP-56 and comparison with known sequences revealed about 60% homology to the adenylate cyclase-associated protein (CAP) from yeast.

Profilin-actin complexes directly elongate actin filaments at the barbed end

We demonstrate that the profilin-G-actin complex can elongate actin filaments directly at the barbed end but cannot bind to the pointed end. During elongation, the profilin-actin complex binds to the barbed filament end, whereupon profilin is released, leaving the actin molecule behind. This was first proposed by Tilney [Tilney, L. G., et al. (1983) J. Cell Biol. 97, 112-124] and demonstrated by Pollard and Cooper [(1984) Biochemistry 23, 6631-6641] by electron microscopy. We show that a model without any outside energy supply, in contrast to the mechanism proposed by Pollard and Cooper, can be fitted to our and their [Kaiser et al. (1986) J. Cell Biol. 102, 221-226] findings. Input of outside energy is necessary only if profilin-mediated elongation continues after free G-actin has been lowered to or below the critical concentration observed at the barbed end in the absence of profilin.

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.

Binding of sugar phosphates, inositol phosphates and phosphorylated amino acids to actin

Binding of biological phosphate compounds to actin was investigated by the effect of these compounds on the critical concentration of the pointed ends of gelsolin-capped actin filaments. According to this assay millimolar concentrations of glucose 6-phosphate and the bisphosphorylated sugars fructose 1,6-bisphosphate, fructose 2,6-bisphosphate, glucose 1,6-bisphosphate, sedoheptulose 1,7-bisphosphate and 2,3-bisphosphoglycerate were found to associate with actin. Glycerophosphoinositol phosphates bound to actin if they were present in millimolar concentrations, and if carbon atom 4 of the inositol ring was phosphorylated and carbon atom 5 was free of phosphate. Also phosphoserine and phosphotyrosine were found to interact with actin. Most of the actin-binding compounds stabilized actin filaments by decreasing the critical concentration suggesting that these compounds had a higher affinity for the subunits along actin filaments than for actin monomers. However, 2,3-bisphosphoglycerate and fructose 2,6-bisphosphate increased the critical concentration probably because these sugar phosphates bound to actin monomers thereby inhibiting actin polymerization.

Mechanism of the insertion of actin monomers between the barbed ends of actin filaments and barbed end-bound insertin

Insertin, a protein purified from chicken gizzard smooth muscle, has been shown to retard but not to inhibit actin polymerization at the barbed ends of actin filaments. This effect has been explained by a model in which insertin remains bound to the barbed ends of actin filaments and new actin molecules are inserted into filaments between the barbed ends and barbed end-bound insertin molecules. In this paper we discuss the mechanism of the insertion reaction on a molecular level. A number of simple models were devised and were judged by their agreement with available experimental data. In one class of models insertin was assumed to dissociate from filament ends and to re-associate with the ends. Actin monomers would then bind to a filament end between a dissociation and an association reaction of insertin. In one of the two proposed models in this class insertin binds to an ATP-containing terminal subunit with higher affinity than to an ADP-containing terminal subunit. Dissociation of insertin is brought about by ATP hydrolysis at the terminal filament subunit. Insertion was then thought to re-associate with a filament end following binding of an ATP-containing actin monomer to the filament end. In the other of the two models' insertin was assumed to occur in two conformations which bind to filament ends with different affinities. Association and dissociation of insertin is caused by interconversion between the two forms of insertin. Both models turned out to be incompatible with experimental data. All types of models in which retardation of actin polymerization is brought about by dissociation and re-association of insertin with filament ends can be excluded by a common argument. As 10 nM insertin retards polymerization of 2 microns monomeric actin with maximal efficiency, the rate constant of binding of insertin to a filament end must be considerably higher (greater than 2 microM/10 nM = 200-fold). As the rate of association of actin with a barbed end is almost diffusion-controlled, assembly of insertin with a filament end would have to exceed the rate of a diffusion-controlled reaction. In the other class of models it was assumed that insertin remains permanently bound to filament ends during association or dissociation of an actin molecule and to move towards the terminal subunit of filaments. These models are compatible with experimental data. Thus, models are favoured where insertin remains bound to filament ends during polymerization and depolymerization of actin.

De-ADP-ribosylation actin by Clostridium perfringens iota-toxin and Clostridium botulinum C2 toxin

The reverse reaction of the ADP-ribosylation of actin by Clostridium botulinum C2 toxin and Clostridium perfringens iota-toxin was studied. In the presence of nicotinamide (30-50 mM) C2 toxin and iota-toxin decreased the radioactive labeling of [32P]ADP-ribosylated actin and catalyzed the formation of [32P]NAD. The pH optima for both reactions were 5.5-6.0. Concomitant with the removal of ADP-ribose, the ability of actin to polymerize was restored and actin ATPase activity increased. Neither ADP-ribosylation nor removal of ADP-ribose was observed after treatment of actin with EDTA, indicating that the native structure of actin is required for both reactions. ADP-ribosylation of platelet actin by C2 toxin was reversed by iota-toxin, confirming recent reports that both toxins modify the same amino acid in actin. However, C. botulinum C2 toxin was not able to cleave ADP-ribose from skeletal muscle actin which had been incorporated by iota-toxin, corroborating the different substrate specificities of both toxins.

Tropomyosin-troponin complex stabilizes the pointed ends of actin filaments against polymerization and depolymerization

In striated muscle the pointed ends of polar actin filaments are directed toward the center of the sarcomere. Formed filaments keep a constant length of about 1 micron. As polymerization and depolymerization at free pointed ends are not sufficiently slow to account for the constant length of the filaments, we searched for proteins which occur in sarcomeres and can stabilize the pointed ends of actin filaments. We observed that tropomyosin-troponin complex reduces the rate of association and dissociation of actin molecules at the pointed ends more than 30-fold. On the average, every 600 s one association or dissociation reaction has been found to occur at the pointed ends near the critical actin monomer concentration.

Kinetic evidence for insertion of actin monomers between the barbed ends of actin filaments and barbed end-bound insertin, a protein purified from smooth muscle

An actin polymerization-retarding protein was isolated from chicken gizzard smooth muscle. This protein copurified with vinculin on DEAE-cellulose and gel filtration columns. The polymerization-retarding protein could be separated from vinculin by hydroxylapatite chromatography. The isolated polymerization-retarding protein lost its activity within a few days, but was stable for weeks when it was not separated from vinculin. We termed the polymerization-retarding protein "insertin". Because of the instability of the isolated insertin, we investigated the effect of insertin-vinculin on actin polymerization. Insertin-vinculin retarded nucleated actin polymerization maximally fivefold. Polymerization at the pointed ends of gelsolin-capped actin filaments was not affected by insertin-vinculin, suggesting that insertin-vinculin binds to the barbed ends, but not to the pointed ends, of actin filaments. Retarded polymerization was observed even if the actin monomer concentration was between the critical concentrations of the ends of treadmilling actin filaments. As at this low monomer concentration the pointed ends depolymerize, monomers appeared to be inserted at the barbed ends between the terminal subunit and barbed end-bound insertin molecules. Insertin-vinculin was found not to increase the actin monomer concentration to the value of the pointed ends. These observations support the conclusion that insertin is not a barbed end-capping protein but an actin monomer-inserting protein. According to a quantitative analysis of the kinetic data, all observations could be explained by a model in which two insertin molecules were assumed to bind co-operatively to the barbed ends of actin filaments. Actin monomers were found to be inserted between the barbed ends and barbed end-bound insertin molecules at a rate of about 1 x 10(6) M-1 s-1. Insertin may be an essential part of the machinery of molecules that permit treadmilling of actin filaments in living cells by insertion of actin molecules between membranes and actin filaments.

Expression of human plasma gelsolin in Escherichia coli and dissection of actin binding sites by segmental deletion mutagenesis

Human plasma gelsolin has been expressed in high yield and soluble form in Escherichia coli. The protein has nucleating and severing activities identical to those of plasma gelsolin and is fully calcium sensitive in its interactions with monomeric actin. A number of deletion mutants have been expressed to explore the function of the three actin binding sites. Their design is based on the sixfold segmental repeat in the protein sequence. (These sites are located in segment 1, segments 2-3, and segments 4-6). Two mutants, S1-3 and S4-6, are equivalent to the NH2- and COOH-terminal halves of the molecule obtained by limited proteolysis. S1-3 binds two actin monomers in the presence or absence of calcium, it severs and caps filaments but does not nucleate polymerization. S4-6 binds a single actin monomer but only in calcium. These observations confirm and extend current knowledge on the properties of the two halves of gelsolin. Two novel constructs have also been studied that provide a different pairwise juxtaposition of the three sites. S2-6, which lacks the high affinity site of segment 1 (equivalent to the 14,000-Mr proteolytic fragment) and S1,4-6, which lacks segments 2-3 (the actin filament binding domain previously identified using the 28,000-Mr proteolytic fragment). S2-6 binds two actin monomers in calcium and nucleates polymerization; it associates laterally with filaments in the presence or absence of calcium and has a weak calcium-dependent fragmenting activity. S1,4-6 also binds two actin monomers in calcium and one in EGTA, has weak severing activity but does not nucleate polymerization. A model is presented for the involvement of the three binding sites in the various activities of gelsolin.

Nonmuscle actin ADP-ribosylated by botulinum C2 toxin caps actin filaments

The effect of nonmuscle actin ADP-ribosylated by botulinum C2 toxin on the polymerization of nonmuscle actin was investigated in order to clarify whether nonmuscle actin is converted into a capping protein by ADP-ribosylation. ADP-ribosylated actin was found to decrease the rate of polymerization of actin filaments which are free at both ends. ADP-ribosylated actin turned out to have no effect on the rate or extent of polymerization at the pointed ends of actin filaments the barbed ends of which were capped by gelsolin. The monomer concentration reached at the final stage of polymerization was similar to the critical concentration of the pointed ends of actin filaments. The results suggest that nonmuscle actin ADP-ribosylated by botulinum C2 toxin acts as a capping protein which binds to the barbed ends to inhibit polymerization.

Accumulation of fluorescently labeled actin in the cortical layer in sea urchin eggs after fertilization

Actin from sea urchin eggs was fluorescently labeled with fluorescein isothiocyanate (FITC), N-(7-dimethylamino-4-methylcoumarinyl)-maleimide (DACM), or 5-iodoacetamidofluorescein (IAF) and microinjected into sea urchin eggs and oocytes. It distributed evenly in the cytoplasm of unfertilized eggs. Upon fertilization, actin accumulated first around the sperm binding site and, soon afterwards, in the fertilization cone. The accumulation propagated all over the cortex after a latent period of 10-20 sec. In the case of Clypeaster japonicus eggs, propagation of the accumulation coincided with a shape change in the egg, suggesting that the accumulated actin in the cortex generates forces. FITC-actin was incorporated into microvilli and retained in the cortex after cleavage. On the other hand, DACM- or IAF-actin was not incorporated into microvilli and was dispersed from the cortex by cleavage. These differences may be attributable to differences in the properties of the actins labeled at different sites. After photobleaching by laser light irradiation, FITC- or IAF-actin redistributed in the cortex of fertilized egg as quickly as it did before fertilization. When an unfertilized egg was injected with both actin and a calcium buffer (intracellular free Ca2+ concentration 9 microM), the actin accumulation was similar to that during fertilization but without the latent period. This suggests that the accumulation depended on the increase in the intracellular free Ca2+ concentration. When the unfertilized egg was injected with 0.2 M EGTA after injection of labeled actin and then inseminated, it accumulated only in the protrusion of cytoplasm where the sperm had entered, and fertilization was not completed. In immature oocytes, the accumulation was observed in the cortical region, including the huge protrusion of the cytoplasm where the sperm had entered. These results suggest that actin accumulation in the sperm binding site plays an important role in the sperm reception mechanism of the egg.

Actin polymerization and ATP hydrolysis

F-actin is the major component of muscle thin filaments and, more generally, of the microfilaments of the dynamic, multifunctional cytoskeletal systems of nonmuscle eukaryotic cells. Polymeric F-actin is formed by reversible noncovalent self-association of monomeric G-actin. To understand the dynamics of microfilament systems in cells, the dynamics of polymerization of pure actin must be understood. The following model has emerged from recent work. During the polymerization process, adenosine 5'-triphosphate (ATP) that is bound to G-actin is hydrolyzed to adenosine 5'-diphosphate (ADP) that is bound to F-actin. The hydrolysis reaction occurs on the F-actin subsequent to the polymerization reaction in two steps: cleavage of ATP followed by the slower release of inorganic phosphate (Pi). As a result, at high rates of filament growth a transient cap of ATP-actin subunits exists at the ends of elongating filaments, and at steady state a stabilizing cap of ADP.Pi-actin subunits exists at the barbed ends of filaments. Cleavage of ATP results in a highly stable filament with bound ADP.Pi, and release of Pi destabilizes the filament. Thus these two steps of the hydrolytic reaction provide potential mechanisms for regulating the monomer-polymer transition.

pH-dependent rate of formation of the gelsolin-actin complex from gelsolin and monomeric actin

The assembly of gelsolin with actin was followed by the increase of the fluorescence intensity of a fluorescence label bound to actin. The time course of the formation of the gelsolin-actin complex in the presence of micromolar [Ca2+] could be quantitatively interpreted by a model in which one actin molecule binds slowly to gelsolin in a rate-determining step and subsequently a second actin molecule is bound at least 40 times more rapidly. The rate of binding of the first actin molecule to gelsolin was found to be remarkably slow and to depend on the pH. The rate constants of formation of the gelsolin-actin complex range from 1.5 X 10(4) M-1 s-1 at pH 8 to 7 X 10(4) M-1 s-1 at pH 6.

Binding of phosphate ions to actin

The decrease of the critical monomer concentration of ADP-actin by millimolar phosphate concentrations has been analysed in terms of equilibrium constants for binding of phosphate ions to ADP-actin. The decrease has been explained by a 10-fold greater affinity of phosphate ions to polymeric ADP-actin (binding constant 100 M-1) than to monomeric ADP-actin (binding constant 10 M-1). Phosphate has an almost identical effect on the critical monomer concentration of the pointed ends of gelsolin-capped actin filaments in the presence of ATP. The phosphate concentration required for half-maximal decrease of the critical monomer concentration of the pointed ends has been determined to be about 15 mM. By using the fluorescent ATP-analogue, 1,N6-ethenoadenosine 5'-triphosphate, phosphate ions have been found to bind also to monomeric ATP-actin, yet with a slightly higher affinity than to monomeric ADP-actin (binding constant 50 M-1).

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.

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.