scholarly journals Actin filaments function as a tension sensor by tension-dependent binding of cofilin to the filament

2011 ◽  
Vol 195 (5) ◽  
pp. 721-727 ◽  
Author(s):  
Kimihide Hayakawa ◽  
Hitoshi Tatsumi ◽  
Masahiro Sokabe
Keyword(s):  
Actin Cytoskeleton ◽  
Optical Tweezers ◽  
Actin Filament ◽  
Actin Filaments ◽  
Stress Fiber ◽  
Mechanical Forces ◽  
Actin Bundle ◽  
Structure And Dynamics ◽  
Binding Rate ◽  
Tension Sensor

Intracellular and extracellular mechanical forces affect the structure and dynamics of the actin cytoskeleton. However, the underlying molecular and biophysical mechanisms, including how mechanical forces are sensed, are largely unknown. Actin-depolymerizing factor/cofilin proteins are actin-modulating proteins that are ubiquitously distributed in eukaryotes, and they are the most likely candidate as proteins to drive stress fiber disassembly in response to changes in tension in the fiber. In this study, we propose a novel hypothesis that tension in an actin filament prevents the filament from being severed by cofilin. To test this, we placed single actin filaments under tension using optical tweezers. When a fiber was tensed, it was severed after the application of cofilin with a significantly larger delay in comparison with control filaments suspended in solution. The binding rate of cofilin to an actin bundle decreased when the bundle was tensed. These results suggest that tension in an actin filament reduces the cofilin binding, resulting in a decrease in its effective severing activity.

scholarly journals Bundling of actin filaments by alpha-actinin depends on its molecular length.

1990 ◽  
Vol 110 (6) ◽  
pp. 2013-2024 ◽  
Author(s):  
R K Meyer ◽  
U Aebi
Keyword(s):  
Smooth Muscle ◽  
Actin Filament ◽  
Actin Filaments ◽  
Actin Binding ◽  
Molar Ratio ◽  
Cross Linking ◽  
Actin Bundle ◽  
Actin Bundles ◽  
Chicken Gizzard ◽  
Molecular Length

Cross-linking of actin filaments (F-actin) into bundles and networks was investigated with three different isoforms of the dumbbell-shaped alpha-actinin homodimer under identical reaction conditions. These were isolated from chicken gizzard smooth muscle, Acanthamoeba, and Dictyostelium, respectively. Examination in the electron microscope revealed that each isoform was able to cross-link F-actin into networks. In addition, F-actin bundles were obtained with chicken gizzard and Acanthamoeba alpha-actinin, but not Dictyostelium alpha-actinin under conditions where actin by itself polymerized into disperse filaments. This F-actin bundle formation critically depended on the proper molar ratio of alpha-actinin to actin, and hence F-actin bundles immediately disappeared when free alpha-actinin was withdrawn from the surrounding medium. The apparent dissociation constants (Kds) at half-saturation of the actin binding sites were 0.4 microM at 22 degrees C and 1.2 microM at 37 degrees C for chicken gizzard, and 2.7 microM at 22 degrees C for both Acanthamoeba and Dictyostelium alpha-actinin. Chicken gizzard and Dictyostelium alpha-actinin predominantly cross-linked actin filaments in an antiparallel fashion, whereas Acanthamoeba alpha-actinin cross-linked actin filaments preferentially in a parallel fashion. The average molecular length of free alpha-actinin was 37 nm for glycerol-sprayed/rotary metal-shadowed and 35 nm for negatively stained chicken gizzard; 46 and 44 nm, respectively, for Acanthamoeba; and 34 and 31 nm, respectively, for Dictyostelium alpha-actinin. In negatively stained preparations we also evaluated the average molecular length of alpha-actinin when bound to actin filaments: 36 nm for chicken gizzard and 35 nm for Acanthamoeba alpha-actinin, a molecular length roughly coinciding with the crossover repeat of the two-stranded F-actin helix (i.e., 36 nm), but only 28 nm for Dictyostelium alpha-actinin. Furthermore, the minimal spacing between cross-linking alpha-actinin molecules along actin filaments was close to 36 nm for both smooth muscle and Acanthamoeba alpha-actinin, but only 31 nm for Dictyostelium alpha-actinin. This observation suggests that the molecular length of the alpha-actinin homodimer may determine its spacing along the actin filament, and hence F-actin bundle formation may require "tight" (i.e., one molecule after the other) and "untwisted" (i.e., the long axis of the molecule being parallel to the actin filament axis) packing of alpha-actinin molecules along the actin filaments.

scholarly journals F-actin bundles in Drosophila bristles are assembled from modules composed of short filaments.

1996 ◽  
Vol 135 (5) ◽  
pp. 1291-1308 ◽  
Author(s):  
L G Tilney ◽  
P Connelly ◽  
S Smith ◽  
G M Guild
Keyword(s):  
Actin Filament ◽  
Actin Filaments ◽  
Modular Design ◽  
Thin Sections ◽  
Actin Bundle ◽  
Actin Bundles ◽  
Phalloidin Staining ◽  
Filament Bundles ◽  
End To End ◽  
As If

The actin bundles in Drosophila bristles run the length of the bristle cell and are accordingly 65 microns (microchaetes) or 400 microns (macrochaetes) in length, depending on the bristle type. Shortly after completion of bristle elongation in pupae, the actin bundles break down as the bristle surface becomes chitinized. The bundles break down in a bizarre way; it is as if each bundle is sawed transversely into pieces that average 3 microns in length. Disassembly of the actin filaments proceeds at the "sawed" surfaces. In all cases, the cuts in adjacent bundles appear in transverse register. From these images, we suspected that each actin bundle is made up of a series of shorter bundles or modules that are attached end-to-end. With fluorescent phalloidin staining and serial thin sections, we show that the modular design is present in nondegenerating bundles. Decoration of the actin filaments in adjacent bundles in the same bristle with subfragment 1 of myosin reveals that the actin filaments in every module have the same polarity. To study how modules form developmentally, we sectioned newly formed and elongating bristles. At the bristle tip are numerous tiny clusters of 6-10 filaments. These clusters become connected together more basally to form filament bundles that are poorly organized, initially, but with time become maximally cross-linked. Additional filaments are then added to the periphery of these organized bundle modules. All these observations make us aware of a new mechanism for the formation and elongation of actin filament bundles, one in which short bundles are assembled and attached end-to-end to other short bundles, as are the vertical girders between the floors of a skyscraper.

scholarly journals Identification of Novel Graded Polarity Actin Filament Bundles in Locomoting Heart Fibroblasts: Implications for the Generation of Motile Force

1997 ◽  
Vol 136 (6) ◽  
pp. 1287-1305 ◽  
Author(s):  
Louise P. Cramer ◽  
Margaret Siebert ◽  
Timothy J. Mitchison
Keyword(s):  
Cell Body ◽  
Actin Filament ◽  
Actin Filaments ◽  
Structural Organization ◽  
Actin Bundle ◽  
Inner Surface ◽  
Filament Bundles ◽  
First Time ◽  
Dynamic Populations ◽  
Uniform Polarity

We have determined the structural organization and dynamic behavior of actin filaments in entire primary locomoting heart fibroblasts by S1 decoration, serial section EM, and photoactivation of fluorescence. As expected, actin filaments in the lamellipodium of these cells have uniform polarity with barbed ends facing forward. In the lamella, cell body, and tail there are two observable types of actin filament organization. A less abundant type is located on the inner surface of the plasma membrane and is composed of short, overlapping actin bundles (0.25–2.5 μm) that repeatedly alternate in polarity from uniform barbed ends forward to uniform pointed ends forward. This type of organization is similar to the organization we show for actin filament bundles (stress fibers) in nonlocomoting cells (PtK2 cells) and to the known organization of muscle sarcomeres. The more abundant type of actin filament organization in locomoting heart fibroblasts is mostly ventrally located and is composed of long, overlapping bundles (average 13 μm, but can reach up to about 30 μm) which span the length of the cell. This more abundant type has a novel graded polarity organization. In each actin bundle, polarity gradually changes along the length of the bundle. Actual actin filament polarity at any given point in the bundle is determined by position in the cell; the closer to the front of the cell the more barbed ends of actin filaments face forward. By photoactivation marking in locomoting heart fibroblasts, as expected in the lamellipodium, actin filaments flow rearward with respect to substrate. In the lamella, all marked and observed actin filaments remain stationary with respect to substrate as the fibroblast locomotes. In the cell body of locomoting fibroblasts there are two dynamic populations of actin filaments: one remains stationary and the other moves forward with respect to substrate at the rate of the cell body. This is the first time that the structural organization and dynamics of actin filaments have been determined in an entire locomoting cell. The organization, dynamics, and relative abundance of graded polarity actin filament bundles have important implications for the generation of motile force during primary heart fibroblast locomotion.

scholarly journals Computing on actin bundles network

2019 ◽  
Vol 9 (1) ◽  
Author(s):  
Andrew Adamatzky ◽  
Florian Huber ◽  
Jörg Schnauß
Keyword(s):  
Actin Filament ◽  
Actin Filaments ◽  
Ionic Currents ◽  
Computational Experiments ◽  
Two Dimensional ◽  
Actin Bundle ◽  
Actin Bundles ◽  
Actin Networks

Abstract Actin filaments are conductive to ionic currents, mechanical and voltage solitons. These travelling localisations can be utilised to generate computing circuits from actin networks. The propagation of localisations on a single actin filament is experimentally unfeasible to control. Therefore, we consider excitation waves propagating on bundles of actin filaments. In computational experiments with a two-dimensional slice of an actin bundle network we show that by using an arbitrary arrangement of electrodes, it is possible to implement two-inputs-one-output circuits.

scholarly journals Mechanisms of actin disassembly

2013 ◽  
Vol 24 (15) ◽  
pp. 2299-2302 ◽  
Author(s):  
William Brieher
Keyword(s):  
Actin Cytoskeleton ◽  
Cell Motility ◽  
Actin Filament ◽  
Actin Filaments ◽  
Actin Polymerization ◽  
Actin Depolymerization ◽  
Filament Dynamics ◽  
Physiological Demands ◽  
In Cells

The actin cytoskeleton is constantly assembling and disassembling. Cells harness the energy of these turnover dynamics to drive cell motility and organize cytoplasm. Although much is known about how cells control actin polymerization, we do not understand how actin filaments depolymerize inside cells. I briefly describe how the combination of imaging actin filament dynamics in cells and using in vitro biochemistry progressively altered our views of actin depolymerization. I describe why I do not think that the prevailing model of actin filament turnover—cofilin-mediated actin filament severing—can account for actin filament disassembly detected in cells. Finally, I speculate that cells might be able to tune the mechanism of actin depolymerization to meet physiological demands and selectively control the stabilities of different actin arrays.

Actin and the coordination of protrusion, attachment and retraction in cell crawling

1996 ◽  
Vol 16 (5) ◽  
pp. 351-368 ◽  
Author(s):  
J. Victor Small ◽  
Kurt Anderson ◽  
Klemens Rottner
Keyword(s):  
Actin Cytoskeleton ◽  
Actin Filament ◽  
Actin Filaments ◽  
Actin Polymerization ◽  
The Other ◽  
Coordination Mechanism ◽  
Over Expression ◽  
Cell Crawling ◽  
Cell Front ◽  
A Cell

To crawl over a substrate a cell must first protrude in front, establish new attachments to the substrate and then retract its rear. Protrusion and retraction utilise different subcompartments of the actin cytoskeleton and operate by different mechanisms, one involving actin polymerization and the other myosin-based contraction. Using as examples the rapidly locomoting keratocyte and the slowly moving fibroblast we illustrate how over expression of one or the other actin subcompartments leads to the observed differences in motility. We also propose, that despite these differences there is a common coordination mechanism underlying the genesis of the actin cytoskeleton that involves the nucleation of actin filaments at the protruding cell front, in the lamellipodium, and the relocation of these filaments, via polymerization and flow, to the more posterior actin filament compartments.

scholarly journals Evolutionarily diverse LIM domain-containing proteins bind stressed actin filaments through a conserved mechanism

2020 ◽  
Author(s):  
Jonathan D. Winkelman ◽  
Caitlin A. Anderson ◽  
Cristian Suarez ◽  
David R. Kovar ◽  
Margaret L. Gardel
Keyword(s):  
Actin Cytoskeleton ◽  
Fission Yeast ◽  
Actin Filaments ◽  
Mammalian Cells ◽  
Stress Fiber ◽  
Stress Fibers ◽  
Strain Sensing ◽  
Lim Domain ◽  
Lim Domains ◽  
Functionally Diverse

SUMMARYThe actin cytoskeleton assembles into diverse load-bearing networks including stress fibers, muscle sarcomeres, and the cytokinetic ring to both generate and sense mechanical forces. The LIM (Lin11, Isl-1 & Mec-3) domain family is functionally diverse, but most members can associate with the actin cytoskeleton with apparent force-sensitivity. Zyxin rapidly localizes via its LIM domains to failing stress fibers in cells, known as strain sites, to initiate stress fiber repair and maintain mechanical homeostasis. The mechanism by which these LIM domains associate with stress fiber strain sites is not known. Additionally, it is unknown how widespread strain sensing is within the LIM protein family. We observe that many, but not all, LIM domains from functionally diverse proteins localize to spontaneous or induced stress fiber strain sites in mammalian cells. Additionally, the LIM domain region from the fission yeast protein paxillin like 1 (Pxl1) also localizes to stress fiber strain sites in mammalian cells, suggesting that the strain sensing mechanism is ancient and highly conserved. Sequence analysis and mutagenesis of the LIM domain region of zyxin indicate a requirement of tandem LIM domains, which contribute additively, for sensing stress fiber strain sites. In vitro, purified LIM domains from mammalian zyxin and fission yeast Pxl1 bind to mechanically stressed F-actin networks but do not associate with relaxed actin filaments. We propose that tandem LIM domains recognize an F-actin conformation that is rare in the relaxed state but is enriched in the presence of mechanical stress.

scholarly journals Cofilin-mediated actin dynamics promotes actin bundle formation during Drosophila bristle development

2016 ◽  
Vol 27 (16) ◽  
pp. 2554-2564 ◽  
Author(s):  
Jing Wu ◽  
Heng Wang ◽  
Xuan Guo ◽  
Jiong Chen
Keyword(s):  
Actin Filament ◽  
Actin Filaments ◽  
Actin Polymerization ◽  
Model System ◽  
Actin Dynamics ◽  
Actin Network ◽  
Loss Of Function ◽  
Actin Bundle ◽  
Actin Bundles

The actin bundle is an array of linear actin filaments cross-linked by actin-bundling proteins, but its assembly and dynamics are not as well understood as those of the branched actin network. Here we used the Drosophila bristle as a model system to study actin bundle formation. We found that cofilin, a major actin disassembly factor of the branched actin network, promotes the formation and positioning of actin bundles in the developing bristles. Loss of function of cofilin or AIP1, a cofactor of cofilin, each resulted in increased F-actin levels and severe defects in actin bundle organization, with the defects from cofilin deficiency being more severe. Further analyses revealed that cofilin likely regulates actin bundle formation and positioning by the following means. First, cofilin promotes a large G-actin pool both locally and globally, likely ensuring rapid actin polymerization for bundle initiation and growth. Second, cofilin limits the size of a nonbundled actin-myosin network to regulate the positioning of actin bundles. Third, cofilin prevents incorrect assembly of branched and myosin-associated actin filament into bundles. Together these results demonstrate that the interaction between the dynamic dendritic actin network and the assembling actin bundles is critical for actin bundle formation and needs to be closely regulated.

scholarly journals Profilin and formin constitute a pacemaker system for robust actin filament growth

eLife ◽  
2019 ◽  
Vol 8 ◽  
Author(s):  
Johanna Funk ◽  
Felipe Merino ◽  
Larisa Venkova ◽  
Lina Heydenreich ◽  
Jan Kierfeld ◽  
...  
Keyword(s):  
Actin Cytoskeleton ◽  
Actin Filament ◽  
Growth Rates ◽  
Actin Filaments ◽  
Mammalian Cells ◽  
Biological Processes ◽  
Muscle Actin ◽  
Cell Morphogenesis ◽  
Actin Networks ◽  
In Cells

The actin cytoskeleton drives many essential biological processes, from cell morphogenesis to motility. Assembly of functional actin networks requires control over the speed at which actin filaments grow. How this can be achieved at the high and variable levels of soluble actin subunits found in cells is unclear. Here we reconstitute assembly of mammalian, non-muscle actin filaments from physiological concentrations of profilin-actin. We discover that under these conditions, filament growth is limited by profilin dissociating from the filament end and the speed of elongation becomes insensitive to the concentration of soluble subunits. Profilin release can be directly promoted by formin actin polymerases even at saturating profilin-actin concentrations. We demonstrate that mammalian cells indeed operate at the limit to actin filament growth imposed by profilin and formins. Our results reveal how synergy between profilin and formins generates robust filament growth rates that are resilient to changes in the soluble subunit concentration.

scholarly journals A Correlative Analysis of Actin Filament Assembly, Structure, and Dynamics

1997 ◽  
Vol 138 (3) ◽  
pp. 559-574 ◽  
Author(s):  
Michel O. Steinmetz ◽  
Kenneth N. Goldie ◽  
Ueli Aebi
Keyword(s):  
Actin Filament ◽  
Divalent Cation ◽  
Actin Filaments ◽  
Metal Ion ◽  
Cation Binding ◽  
Polymerization Reaction ◽  
Structure And Dynamics ◽  
Filament Assembly ◽  
Cation Binding Site ◽  
Assembly Structure

The effect of the type of metal ion (i.e., Ca2+, Mg2+, or none) bound to the high-affinity divalent cation binding site (HAS) of actin on filament assembly, structure, and dynamics was investigated in the absence and presence of the mushroom toxin phalloidin. In agreement with earlier reports, we found the polymerization reaction of G-actin into F-actin filaments to be tightly controlled by the type of divalent cation residing in its HAS. Moreover, novel polymerization data are presented indicating that LD, a dimer unproductive by itself, does incorporate into growing F-actin filaments. This observation suggests that during actin filament formation, in addition to the obligatory nucleation– condensation pathway involving UD, a productive filament dimer, a facultative, LD-based pathway is implicated whose abundance strongly depends on the exact polymerization conditions chosen. The “ragged” and “branched” filaments observed during the early stages of assembly represent a hallmark of LD incorporation and might be key to producing an actin meshwork capable of rapidly assembling and disassembling in highly motile cells. Hence, LD incorporation into growing actin filaments might provide an additional level of regulation of actin cytoskeleton dynamics. Regarding the structure and mechanical properties of the F-actin filament at steady state, no significant correlation with the divalent cation residing in its HAS was found. However, compared to native filaments, phalloidin-stabilized filaments were stiffer and yielded subtle but significant structural changes. Together, our data indicate that whereas the G-actin conformation is tightly controlled by the divalent cation in its HAS, the F-actin conformation appears more robust than this variation. Hence, we conclude that the structure and dynamics of the Mg–F-actin moiety within the thin filament are not significantly modulated by the cyclic Ca2+ release as it occurs in muscle contraction to regulate the actomyosin interaction via troponin.

Sign in / Sign up

Export Citation Format

Share Document