Viscoelasticity of F-actin and F-actin/gelsolin complexes

Actin is the major protein of eukaryote peripheral cytoplasm where its mechanical effects could determine cell shape and motility. The mechanical properties of purified F-actin, whether it is a viscoelastic fluid or an elastic solid, have been a subject of controversy. Mainstream polymer theory predicts that filaments as long as those found in purified F-actin are so interpenetrated as to appear immobile in measurements over a reasonable time with available instrumentation and that the fluidity of F-actin could only be manifest if the filaments were shortened. We show that the static and dynamic elastic moduli below a critical degree of shear strain are much higher than previously reported, consistent with extreme interpenetration, but that higher strain or treatment with very low concentrations of the F-actin severing protein gelsolin greatly diminish the moduli and cause F-actin to exhibit rheologic behavior expected for independent semidilute rods, and defined by the dimensions of the filaments, including shear rate independent viscosity below a critical shear rate. The findings show that shortening of actin filaments sufficiently to permit reasonable measurements brings out their viscoelastic fluid properties. Since gelsolin shortens F-actin, it is likely that the effect of high strain is also to fragment a population of long actin filaments. We confirmed recent findings that the viscosity of F-actin is inversely proportional to the shear rate, consistent with an indeterminate fluid, but found that gelsolin abolishes this unusual shear rate dependence, indicating that it results from filament disruption during the viscosity measurements.(ABSTRACT TRUNCATED AT 250 WORDS)     

Thermal torsion of F-actin

The equipartition theorem is used to calculate the mode amplitudes for F-actin thermal torsion. The amplitudes phi n are found to scale as n-1, (EI)-1/2, and L1/2, where n is mode number, EI is actin bending stiffness, and L is filament length. Depending on conditions, the amplitude can be as large as 15 degrees; this is discussed briefly in terms of skeletal muscle mechanics.     

Transiently crosslinked F-actin bundles

F-actin bundles are prominent cytoskeletal structures in eukaryotes. They provide mechanical stability in stereocilia, microvilli, filopodia, stress fibers and the sperm acrosome. Bundles are typically stabilized by a wide range of specific crosslinking proteins, most of which exhibit off-rates on the order of 1s⁻¹. Yet F-actin bundles exhibit structural and mechanical integrity on time scales that are orders of magnitude longer. By applying large deformations to reconstituted F-actin bundles using optical tweezers, we provide direct evidence of their differential mechanical response in vitro: bundles exhibit fully reversible, elastic response on short time scales and irreversible, elasto-plastic response on time scales that are long compared to the characteristic crosslink dissociation time. Our measurements show a broad range of characteristic relaxation times for reconstituted F-actin bundles. This can be reconciled by considering that bundle relaxation behavior is also modulated by the number of filaments, crosslinking type and occupation number as well as the consideration of defects due to filament ends.     

Diphasic transformations of F-actin. Effects of urea and MgCl2 on F-actin.

Asakura, Taniguchi and Oosawa [1]proposed that muscle actin polymer under sonic vibration is in a different state from that of the ordinary double stranded helical structure (F-actin), characterised by partially interrupted structures of F-actin, a state of "f-actin". In order to confirm different states for actin polymers [1, 2], physicochemical studies were made by measurements of viscosity, flow birefringence, electric birefringence, fluorescence, electron microscopy, quasielastic light scattering and ATP splitting. The following results were obtained. (1) F-actin polymers can undergo two processes of depolymerization upon treatment with urea and various salts as judged by measurements of flow birefringence and viscosity: one is a rapid process in a solution containing K+ or Ca2+ and urea; the other is a slow process following a brief rapid one in a solution containing Mg2+ and urea. (2) In the presence of Mg2+ and a suitable concentration of urea, F-actin (FMU-actin) appeared to exhibit different properties than ordinary F-actin; it had lower viscosity and lower flow birefringence and it had on the whole a more flexible polymer structure, also judging from experiments of quasielastic light scattering, electric birefringence. The different structure was confirmed directly be electron microscopic observation. The aromatic side chains of FMU-actin were also more mobile than those of F-actin judging from fluorescence measurements. The transformation between F-actin and FMU-actin was reversible. (3) The state of FMU-actin polymers was also characterized by ATP splitting; FMU-actin split about one mole of ATP into ADP and inorganic phosphate per mole of actin monomer at room temperature, where F-actin did not. A molar excess of Mg2+ with respect to actin monomer at room temperature, where F-actin did not. A molar excess of Mg2+ with respect to actin monomer is required for ATP splitting. F-actin in solutions containing K+ or Ca2+ and urea did not split ATP. FMU-actin activated on Mg-ATP-ase of myosin at nearly the same rate as that of F-actin. (4) We have postulated a flexible filament model (f-actin). The relationships between the structure of f-actin and its functional role for force generation during contraction are discussed.     

F-actin aggregates in transformed cells

Polymerized actin has been found aggregated into distinctive patches inside transformed cells in culture. The F-actin-specific fluorescent probe, nitrobenzoxadiazole-phallacidin, labels these F-actin aggregates near the ventral cell surface of cells transformed by RNA or DNA tumor viruses, or by chemical mutagens, or spontaneously. Their appearance in all eight transformed cell types studied suggests their ubiquity and involvement in transformation morphology. Actin patches developed in normal rat kidney (NRK) cells transformed by a temperature-sensitive mutant of Rous sarcoma virus (LA23-NRK) within 30 min after a shift from the nonpermissive (39 degrees C) to the permissive temperature (32 degrees C). Patch appearance paralleling viral src gene expression tends to implicate pp60src kinase activity in destabilizing the cytoskeleton. However, appearance of the actin aggregates in cells not transformed by retrovirus calls for alternative mechanisms, perhaps involving an endogenous kinase, for this apparently common trait.     

Cross-linking constraints on F-actin structure

The DNase I binding loop (residues 38-52), the hydrophobic plug (residues 262-274), and the C terminus region are among the structural elements of monomeric (G-) actin proposed to form the intermonomer interface in F-actin. To test the proximity and interactions of these elements and to provide constraints on models of F-actin structure, cysteine residues were introduced into yeast actin either at residue 41 or 265. These mutations allowed for specific cross-linking of F-actin between C41 and C265, C265 and C374, and C41 and C265 using dibromobimane and disulfide bond formation. The cross-linked products were visualized on SDS-PAGE and by electron microscopy. Model calculations carried out for the cross-linked F-actins revealed that considerable flexibility or displacement of actin residues is required in the disulfide cross-linked segments to fit these filaments into model F-actin structures. The calculated, cross-linked structures showed a better fit to the Holmes rather than the refined Lorenz model of F-actin. It is predicted on the basis of such calculations that image reconstruction of electron micrographs of disulfide cross-linked C41-C374 F-actin should provide a conclusive test of these two similar models of F-actin structure.     

Dynamics of F-actin and F-actin/filamin networks as studied by photon correlation spectroscopy

Photon correlation spectroscopy was used to study both F-actin and F-actin/filamin networks in solution. The measured autocorrelation functions were analyzed with the inverse Laplace transform CONTIN. The resulting frequency distributions consist of maximal five relatively narrow peaks. This rather unexpected finding disagrees with the frequency spectra calculated for an entangled rigid rod model. For this model, we expect spectra consisting of a single broad peak. Factors like flexibility, deviation from an experimental length distribution, interference with chemical reactions, and translation-rotation coupling that would influence the profile of the frequency distribution could be excluded by comparison of the data with model calculations or qualitative estimates. We conclude that our data for F-actin are consistent with the dynamics of an infinite network stable on the time scale of the observed modes. Further support for this interpretation is provided by a comparison with frequency spectra of actin/filamin networks. These appear to be very similar in shape. The main peak of these spectra that corresponds to the slow motions shifts to lower frequencies with increasing cross-link density. It appears that higher frequency modes of the gel are more efficiently damped with progressive cross-link density, resulting in a predominance of the slow motions in the spectra. This behavior has been already found in other systems and seems to be a general feature of cross-linked systems.     

Development of a fluorescent F-actin blot overlay assay for detection of F-actin binding proteins

Interactions between cellular proteins and filamentous (F) actin are key to many cellular functions, e.g., cell motility, endocytosis, cell:cell adhesion, and cell:substrate adhesion. Previously, a functional assay using 125I-labeled F-actin to detect a subset of F-actin binding proteins by blot overlay was developed. We have modified this assay to use the fluorescent label, Alexa 488, in place of 125Iodine. The detection limit for Alexa 488-labeled actin using a Molecular Dynamics STORM 860 Fluorescence/PhosphorImager was as little as 100pg of labeled actin. The Alexa 488 F-actin assay detects the same proteins from Dictyostelium discoideum and with approximately the same sensitivity (approximately 10 microg/ml F-actin final concentration) as the analogous 125I-labeled F-actin blot overlay. The use of Alexa 488 F-actin for blot overlay assays requires no radioactive materials and generates no hazardous waste. Assays can be performed on the laboratory bench top and the blots imaged directly with a blue laser scanner, either wet or dry. In addition, the Alexa 488 fluorophore is highly resistant to photobleaching, does not decay, and may be stored frozen or lyophilized. Alexa 488 F-actin is a stable, cost-effective, nonhazardous probe used for rapid identification of a subset of F-actin binding proteins.     

Mechanics of the F-actin cytoskeleton

Dynamic regulation of the filamentous actin (F-actin) cytoskeleton is critical to numerous physical cellular processes, including cell adhesion, migration and division. Each of these processes require precise regulation of cell shape and mechanical force generation which, to a large degree, is regulated by the dynamic mechanical behaviors of a diverse assortment of F-actin networks and bundles. In this review, we review the current understanding of the mechanics of F-actin networks and identify areas of further research needed to establish physical models. We first review our understanding of the mechanical behaviors of F-actin networks reconstituted in vitro, with a focus on the nonlinear mechanical response and behavior of “active” F-actin networks. We then explore the types of mechanical response measured of cytoskeletal F-actin networks and bundles formed in living cells and identify how these measurements correspond to those performed on reconstituted F-actin networks formed in vitro. Together, these approaches identify the challenges and opportunities in the study of living cytoskeletal matter.     

Fluorescence anisotropy of labelled F-actin: Influence of Ca2+ on the flexibility of F-actin

We measured the fluorescence static anisotropy and the time-resolved fluorescence anisotropy decay of F-actin labelled with N-iodoacetyl-N'-(5-sulfo-1-naphthyl)ethylenediamine at 20°C in solutions containing 100 mM KCl and free Ca²⁺ at various concentrations. The average fluorescence anisotropy and the fluorescence rotational correlation time of actin decreased in the presence of micromolar concentrations of free Ca²⁺. The change of the rotational correlation time of labelled actin could not be explained by a variation of the actin critical concentration. We concluded therefore that F-actin undergoes a conformational change induced by Ca²⁺ binding. The binding constant was 6 × 10⁶ M^?1.     

Isolation of F-actin from pea stems

Summary A procedure is introduced which allows the isolation of abundant amounts of F-actin from plants (etiolated pea seedlings) in an array of morphologies very similar to the array of morphologies found in situ. The major feature is a homogenizing medium containing very low ionic strength, low monovalent ion (K⁺) concentration, a 3-fold higher level of Mg^{+ +}, the presence of EGTA to chelate Ca⁺⁺, and PMSF to inhibit protease activity. Using this buffer, about 80–90% of the sedimentable actin is found in the low speed (4,000×g) pellet.Abbreviations CSB cytoskeleton-isolation buffer - DTE dithioery-thritol - EGTA ethylene-glycol-bis(B-aminoethyl ether) N,N,NN-tetraacetic acid - EPPS N-[2-hydroxyethyl]-piperazine-N-[3-propane-sulfonic acid] - HEPES N-[hydroxyethyl]-piperazine-N-[2-ethanesulfonic acid] - MFSB microfilament-stabilizing buffer - PIPES piperazine-N,N-bis[2-ethanesulfonic acid] - PMSF phenylmethyl-sulfonyl fluoride - PTE polyoxyethylene-10-tridecyl ether - TRIS tris-(hydroxymethyl) aminoethane