Dendritic organization of actin comet tails

Polymerization of actin filaments is necessary for both protrusion of the leading edge of crawling cells and propulsion of certain intracellular pathogens, and it is sufficient for generating force for bacterial motility in vitro. Motile intracellular pathogens are associated with actin-rich comet tails containing many of the same molecular components present in lamellipodia, and this suggests that these two systems use a similar mechanism for motility. However, available structural evidence suggests that the organization of comet tails differs from that of lamellipodia. Actin filaments in lamellipodia form branched arrays, which are thought to arise by dendritic nucleation mediated by the Arp2/3 complex. In contrast, comet tails have been variously described as consisting of short, randomly oriented filaments, with a higher degree of alignment at the periphery, or as containing long, straight axial filaments with a small number of oblique filaments. Because the assembly of pathogen-associated comet tails has been used as a model system for lamellipodial protrusion, it is important to resolve this apparent discrepancy. Here, using a platinum replica approach, we show that actin filament arrays in comet tails in fact have a dendritic organization with the Arp2/3 complex localizing to Y-junctions as in lamellipodia. Thus, comet tails and lamellipodia appear to share a common dendritic nucleation mechanism for protrusive motility. However, comet tails differ from lamellipodia in that their actin filaments are usually twisted and appear to be under significant torsional stress.     

Rapid actin monomer-insensitive depolymerization of Listeria actin comet tails by cofilin, coronin, and Aip1

Actin filaments in cells depolymerize rapidly despite the presence of high concentrations of polymerizable G actin. Cofilin is recognized as a key regulator that promotes actin depolymerization. In this study, we show that although pure cofilin can disassemble Listeria monocytogenes actin comet tails, it cannot efficiently disassemble comet tails in the presence of polymerizable actin. Thymus extracts also rapidly disassemble comet tails, and this reaction is more efficient than pure cofilin when normalized to cofilin concentration. By biochemical fractionation, we identify Aip1 and coronin as two proteins present in thymus extract that facilitate the cofilin-mediated disassembly of Listeria comet tails. Together, coronin and Aip1 lower the amount of cofilin required to disassemble the comet tail and permit even low concentrations of cofilin to depolymerize actin in the presence of polymerizable G actin. The cooperative activities of cofilin, coronin, and Aip1 should provide a biochemical basis for understanding how actin filaments can grow in some places in the cell while shrinking in others.     

Yogi Berra, Forrest Gump, and the discovery of Listeria actin comet tails

In 1988, eminent cell biologist Lew Tilney and newly appointed Assistant Professor of Microbiology Dan Portnoy met at a picnic and initiated a collaboration that led to a groundbreaking paper published in Journal of Cell Biology entitled "Actin filaments and the growth, movement, and spread of the intracellular bacterial parasite, Listeria monocytogenes." The paper has been cited more than 800 times, the most of any publication in the careers of both investigators. Using an electron microscope from the Sputnik era, they assembled a stunning collection of micrographs that illustrated how L. monocytogenes enters the host cell and exploits a host system of actin-based motility to move within cells and into neighboring cells without leaving the host cell cytosol. This research captured the imagination of cell biologists and microbiologists alike and led to novel insights into cytoskeletal dynamics. Here, Portnoy provides a retrospective that shares text from the original submission that was deleted at the time of publication, along with reviewers' comments ranging from "It is really just a show and tell paper and doesn';t have any meat" to "the finding will have major impact in cell biology and in medicine. Potentially, the paper will be a classic."     

Listeria comet tails: the actin-based motility machinery at work

Listeria monocytogenes is a master of mimicry that uses the host cell actin system both to move within the cytoplasm of infected cells and for cell-to-cell spread. Recent studies of Listeria and similarly acting pathogens have generated leaps in our understanding of the actin-based force producing machinery. This machinery is essential for most motile properties of cells, not least for cell migration. In a minimal configuration, it consists of the Arp2/3-complex, Ena-VASP proteins, cofilin, capping protein and a nucleation-promoting factor. In this review, we discuss current models of pseudopodial protrusions and describe how the road to more complex models lies open and is already paved by recent studies using Listeria-based biomimetic motility assays.     

The actin propulsive machinery: the proteome of Listeria monocytogenes tails

Actin-based comet tails produced by Listeria monocytogenes are considered as representative models for cellular force-producing machineries crucial for cell migration. We here present a proteomic picture of these tails formed in extracts from brain and platelets. This provides a comprehensive view, revealing high molecular complexity and novel host cell proteins as tail components, and suggests the participation of specific multicomponent regulatory complexes. This work forms a new basis to expand current models of cellular protrusion.     

Fascin and VASP synergistically increase the Young's modulus of actin comet tails

Cell motility is locally achieved by the interplay between lamellipodia and filopodia at the protrusion sites. The actin cytoskeleton rearranges from a highly branched short filamentous network to well aligned elongated bundles from lamellipodia to filopodia, respectively. This process is governed predominantly by actin binding proteins, VASP and fascin, at the leading edge of migratory cells. Here we use an Arp2/3-complex dependent bead motility assay to study the effect of fascin both on its own and in the presence of VASP. The Young's modulus of phalloidin stabilized comets grown in the presence of fascin increased linearly with concentration above a 0.5 μM threshold. Inversely, the initial velocity of the comets decreased linearly with fascin concentration above the same threshold. Interestingly, VASP and fascin together increased the Young's modulus of the comets compared to those grown in the presence of only one of the two proteins. This effect was most remarkable at low concentration, below 0.5 and 0.15 μM for fascin and VASP, respectively. Our results showed that fascin and VASP work cooperatively to enhance the Young's modulus of the actin network within the comets.     

A mathematical model of actin filament turnover for fitting FRAP data

A novel mathematical model of the actin dynamics in living cells under steady-state conditions has been developed for fluorescence recovery after photobleaching (FRAP) experiments. As opposed to other FRAP fitting models, which use the average lifetime of actins in filaments and the actin turnover rate as fitting parameters, our model operates with unbiased actin association/dissociation rate constants and accounts for the filament length. The mathematical formalism is based on a system of stochastic differential equations. The derived equations were validated on synthetic theoretical data generated by a stochastic simulation algorithm adapted for the simulation of FRAP experiments. Consistent with experimental findings, the results of this work showed that (1) fluorescence recovery is a function of the average filament length, (2) the F-actin turnover and the FRAP are accelerated in the presence of actin nucleating proteins, (3) the FRAP curves may exhibit both a linear and non-linear behaviour depending on the parameters of actin polymerisation, and (4) our model resulted in more accurate parameter estimations of actin dynamics as compared with other FRAP fitting models. Additionally, we provide a computational tool that integrates the model and that can be used for interpretation of FRAP data on actin cytoskeleton.     

How Listeria exploits host cell actin to form its own cytoskeleton. II. Nucleation, actin filament polarity, filament assembly, and evidence for a pointed end capper

Processes such as cell locomotion and morphogenesis depend on both the generation of force by cytoskeletal elements and the response of the cell to the resulting mechanical loads. Many widely accepted theoretical models of processes involving cell shape change are based on untested hypotheses about the interaction of these two components of cell shape change. I have quantified the mechanical responses of cytoplasm to various chemical environments and mechanical loading regimes to understand better the mechanisms of cell shape change and to address the validity of these models. Measurements of cell mechanical properties were made with strands of cytoplasm submerged in media containing detergent to permeabilize the plasma membrane, thus allowing control over intracellular milieu. Experiments were performed with equipment that generated sinusoidally varying length changes of isolated strands of cytoplasm from Physarum polycephalum. Results indicate that stiffness, elasticity, and viscosity of cytoplasm all increase with increasing concentration of Ca2+, Mg2+, and ATP, and decrease with increasing magnitude and rate of deformation. These results specifically challenge assumptions underlying mathematical models of morphogenetic events such as epithelial folding and cell division, and further suggest that gelation may depend on both actin cross-linking and actin polymerization.     

Quantitative analysis of the effect of Acanthamoeba profilin on actin filament nucleation and elongation

The current view of the mechanism of action of Acanthamoeba profilin is that it binds to actin monomers, forming a complex that cannot polymerize [Tobacman, L. S., & Korn, E. D. (1982) J. Biol. Chem. 257, 4166-4170; Tseng, P., & Pollard, T. D. (1982) J. Cell Biol. 94, 213-218; Tobacman, L. S., Brenner, S. L., & Korn, E. D. (1983) J. Biol. Chem. 258, 8806-8812]. This simple model fails to predict two new experimental observations made with Acanthamoeba actin in 50 mM KC1, 1 mM MgCl2, and 1 mM EGTA. First, Acanthamoeba profilin inhibits elongation of actin filaments far more at the pointed end than at the barbed end. According, to the simple model, the Kd for the profilin-actin complex is less than 5 microM on the basis of observations at the pointed end and greater than 50 microM for the barbed end. Second, profilin inhibits nucleation more strongly than elongation. According to the simple model, the Kd for the profilin-actin complex is 60-140 microM on the basis of two assays of elongation but 2-10 microM on the basis of polymerization kinetics that reflect nucleation. These new findings can be explained by a new and more complex model for the mechanism of action that is related to a proposal of Tilney and co-workers [Tilney, L. G., Bonder, E. M., Coluccio, L. M., & Mooseker, M. S. (1983) J. Cell Biol. 97, 113-124]. In this model, profilin can bind both to actin monomers with a Kd of about 5 microM and to the barbed end of actin filaments with a Kd of about 50-100 microM. An actin monomer bound to profilin cannot participate in nucleation or add to the pointed end of an actin filament. It can add to the barbed end of a filament. When profilin is bound to the barbed end of a filament, actin monomers cannot bind to that end, but the terminal actin protomer can dissociate at the usual rate. This model includes two different Kd's--one for profilin bound to actin monomers and one for profilin bound to an actin molecule at the barbed end of a filament. The affinity for the end of the filament is lower by a factor of 10 than the affinity for the monomer, presumably due to the difference in the conformation of the two forms of actin or to steric constraints at the end of the filament.     

Insulin stimulates actin comet tails on intracellular GLUT4-containing compartments in differentiated 3T3L1 adipocytes

Incubation of isolated GLUT4-containing vesicles with Xenopus oocyte extracts resulted in a guanosine 5'-[gamma-thio]triphosphate (GTP gamma S) and sodium orthovanadate stimulation of actin comet tails. The in vitro actin-based GLUT4 vesicle motility was inhibited by both latrunculin B and a dominant-interfering N-WASP mutant, N-WASP/Delta VCA. Preparations of gently sheared (broken) 3T3L1 adipocytes also displayed GTP gamma S and sodium orthovanadate stimulation of actin comet tails on GLUT4 intracellular compartments. Furthermore, insulin pretreatment of intact adipocytes prior to gently shearing also resulted in a marked increase in actin polymerization and actin comet tailing on GLUT4 vesicles. In addition, the insulin stimulation of actin comet tails was completely inhibited by Clostridum difficile toxin B, demonstrating a specific role for a Rho family member small GTP-binding protein. Expression of N-WASP/Delta VCA in intact cells had little effect on adipocyte cortical actin but partially inhibited insulin-stimulated GLUT4 translocation. Taken together, these data demonstrate that insulin can induce GLUT4 vesicle actin comet tails that are necessary for the efficient translocation of GLUT4 from intracellular storage sites to the plasma membrane.     

Biochemical analysis of actin in crane-fly gonial cells: evidence for actin in spermatocytes and spermatids--but not sperm

A biochemical assay employing DNase-I affinity chromatography, two- dimensional peptide analysis and SDS polyacrylamide gel electrophoresis was used to isolate, identify, and assess the amount of actin from gonial cells of the crane fly, Nephrotoma suturalis. Based on the analysis of cell homogenates under conditions in which all cellular actin is converted to the monomeric DNase-binding form, actin comprises approximately 1% of the total protein in homogenates of spermatocytes and spermatids. SDS gel analysis of mature sperm reveals no polypeptides with a molecular weight similar to that of actin. Under conditions that preserve native supramolecular states of actin, approximately 80% of the spermatocyte actin is in a sedimentable form whereas only approximately 30% of the spermatid actin is sedimentable. These differences could be meaningful with regard to strutural changes that occur during spermiogenesis. A comparative analysis of two- dimensional peptide maps of several radioiodinated actins reveals similarities among spermatocyte, spermatid, and human erythrocyte actins. The results suggest the general applicability of this approach to other cell types that contain limited amounts of actin.     

Role for actin filament turnover and a myosin II motor in cytoskeleton-driven disassembly of the epithelial apical junctional complex

Disassembly of the epithelial apical junctional complex (AJC), composed of the tight junction (TJ) and adherens junction (AJ), is important for normal tissue remodeling and pathogen-induced disruption of epithelial barriers. Using a calcium depletion model in T84 epithelial cells, we previously found that disassembly of the AJC results in endocytosis of AJ/TJ proteins. In the present study, we investigated the role of the actin cytoskeleton in disassembly and internalization of the AJC. Calcium depletion induced reorganization of apical F-actin into contractile rings. Internalized AJ/TJ proteins colocalized with these rings. Both depolymerization and stabilization of F-actin inhibited ring formation and disassembly of the AJC, suggesting a role for actin filament turnover. Actin reorganization was accompanied by activation (dephosphorylation) of cofilin-1 and its translocation to the F-actin rings. In addition, Arp3 and cortactin colocalized with these rings. F-actin reorganization and disassembly of the AJC were blocked by blebbistatin, an inhibitor of nonmuscle myosin II. Myosin IIA was expressed in T84 cells and colocalized with F-actin rings. We conclude that disassembly of the AJC in calcium-depleted cells is driven by reorganization of apical F-actin. Mechanisms of such reorganization involve cofilin-1-dependent depolymerization and Arp2/3-assisted repolymerization of actin filaments as well as myosin IIA-mediated contraction.     

Quantitative analysis of actin patch movement in yeast

To investigate the mechanism of cortical actin patch movement in yeast, we implement a method for computer tracking the motion of the patches. Digital images from fluorescence microscope movies of living cells are fed into an image-processing program, which generates two-dimensional patch coordinates in the plane of focus for each movie frame via an algorithm based on detection of rapid intensity variations. The patch coordinates in neighboring frames are connected by a minimum-distance algorithm. The method is used to analyze control cells and cells treated with the actin-depolymerizing agent latrunculin. The motion of the patches in both cases, as analyzed by mean-square patch displacements, is found to be a random walk on average, with a much lower diffusion coefficient for the latrunculin-treated cells. The mean-squared patch travel distances for all of the latrunculin-treated cells are lower than those for all of the control cells. The patches move independently of one another. We develop a quantitative criterion for the presence of directed motion, and show that numerous patches in the control cells display directed motion to a very high degree of certainty. A small number of patches in the latrunculin-treated cells display directed motion.     

A theoretical analysis of filament length fluctuations in actin and other polymers

Control of the structure and dynamics of the actin cytoskeleton is essential for cell motility and for maintaining the structural integrity of cells. Central to understanding the control of these features is an understanding of the dynamics of actin filaments, first as isolated filaments, then as integrated networks, and finally as networks containing higher-order structures such as bundles, stress fibers and acto-myosin complexes. It is known experimentally that single filaments can exhibit large fluctuations, but a detailed understanding of the transient dynamics involved is still lacking. Here we first study stochastic models of a general system involving two-monomer types that can be analyzed completely, and then we report stochastic simulations on the complete actin model with three monomer types. We systematically examine the transient behavior of filament length dynamics so as to gain a better understanding of the time scales involved in reaching a steady state. We predict the lifetime of a cap of one monomer type and obtain the mean and variance of the survival time of a cap at the filament end, which together determine the filament length fluctuations.     

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.     

Identification of two regions in the N-terminal domain of ActA involved in the actin comet tail formation by Listeria monocytogenes.

The ActA protein of Listeria monocytogenes induces actin nucleation on the bacterial surface. The continuous process of actin filament elongation provides the driving force for bacterial propulsion in infected cells or cytoplasmic extracts. Here, by fusing the N-terminus of ActA (residues 1-234) to the omega fragment of beta-galactosidase, we present the first evidence that this domain contains all the necessary elements for actin tail formation. A detailed analysis of ActA variants, in which small fragments of the N-terminal region were deleted, allowed the identification of two critical regions. Both are required to initiate the actin polymerization process, but each has in addition a specific role to maintain the dynamics of the process. The first region (region T, amino acids 117-121) is critical for filament elongation, as shown by the absence of actin tail in a 117-121 deletion mutant or when motility assays are performed in the presence of anti-region T antibodies. The second region (region C, amino acids 21-97), is more specifically involved in maintenance of the continuity of the process, probably by F-actin binding or prevention of barbed end capping, as strongly suggested by both a deletion (21-97) leading to 'discontinuous' actin tail formation and in vitro experiments showing that a synthetic peptide covering residues 33-74 can interact with F-actin. Our results provide the first insights in the molecular dissection of the actin polymerization process induced by the N-terminal domain of ActA.     

Regulation of the interaction between actin and myosin subfragment 1: evidence for three states of the thin filament.

Equilibrium titrations and kinetic experiments were used to define the cooperative binding of myosin subfragment 1 (S1) to actin-troponin-tropomyosin. Both types of experiment require an equilibrium between two states of the thin filament in which one state (the off state) binds S1 less readily than the other. Equilibrium titrations are compatible with > 95% of the actin7.Tn.Tm units being in the off state in the absence of calcium and 80% in the off state in the presence of calcium. Kinetic binding data suggest that the presence of calcium switches the thin filament from 70% in the off state to < 5%. The two experiments, therefore, define quite different populations of the off states. We propose a three-state model of the thin filament. A "blocked state" which is unable to bind S1, a "closed state" which can only bind S1 relatively weakly and an "open state" in which the S1 can both bind and undergo an isomerization to a more strongly bound rigor-like conformation. The equilibrium between the three states is calcium-dependent; KB = [closed]/[blocked] = 0.3 and > or = 16 and KT = [open]/[closed] = 0.09 and 0.25 in the absence and presence of calcium, respectively. This model can account for both types of experimental data.     

Quantitative analysis of extension-torsion coupling of actin filaments

Actin filaments have a double-helix structure consisting of globular actin molecules. In many mechanical cellular activities, such as cell movement, division, and shape control, modulation of the extensional and torsional dynamics of the filament has been linked to regulatory actin-binding protein functions. Therefore, it is important to quantitatively evaluate extension-torsion coupling of filament to better understand the actin filament dynamics. In the present study, the extension-torsion coupling was investigated using molecular dynamics simulations. We constructed a model for the actin filament consisting of 14 actin subunits in an ionic solvent as a minimal functional unit, and analyzed longitudinal and twisting Brownian motions of the filament. We then derived the expected value of energy associated with extension and torsion at equilibrium, and evaluated the extension-torsion stiffness of the filament from the thermal fluctuations obtained from the MD simulations. The results demonstrated that as the analyzed sampling-window duration was increased, the extension-torsion coupling stiffness evaluated on a nanosecond scale tended to converge to a value of 7.6×10(-11) N. The results obtained from this study will contribute to the understanding of biomechanical events, under mechanical tension and torque, involving extension-torsion coupling of filaments.