scholarly journals Cease-fire at the leading edge: New perspectives on actin filament branching, debranching, and cross-linking

Cytoskeleton ◽  
2011 ◽  
Vol 68 (11) ◽  
pp. 596-602 ◽  
Author(s):  
Casey A. Ydenberg ◽  
Benjamin A. Smith ◽  
Dennis Breitsprecher ◽  
Jeff Gelles ◽  
Bruce L. Goode
Keyword(s):  
Actin Filament ◽  
Leading Edge ◽  
Cross Linking

scholarly journals Arp2/3 Complex from Acanthamoeba Binds Profilin and Cross-links Actin Filaments

1998 ◽  
Vol 9 (4) ◽  
pp. 841-852 ◽  
Author(s):  
R. Dyche Mullins ◽  
Joseph F. Kelleher ◽  
James Xu ◽  
Thomas D. Pollard
Keyword(s):  
Actin Filament ◽  
Actin Filaments ◽  
Analytical Ultracentrifugation ◽  
Acanthamoeba Castellanii ◽  
Leading Edge ◽  
Actin Binding ◽  
Cross Linking ◽  
Motile Cells ◽  
Mechanism Of Interaction ◽  
Cross Links

The Arp2/3 complex was first purified from Acanthamoeba castellanii by profilin affinity chromatography. The mechanism of interaction with profilin was unknown but was hypothesized to be mediated by either Arp2 or Arp3. Here we show that the Arp2 subunit of the complex can be chemically cross-linked to the actin-binding site of profilin. By analytical ultracentrifugation, rhodamine-labeled profilin binds Arp2/3 complex with a Kd of 7 μM, an affinity intermediate between the low affinity of profilin for barbed ends of actin filaments and its high affinity for actin monomers. These data suggest the barbed end of Arp2 is exposed, but Arp2 and Arp3 are not packed together in the complex exactly like two actin monomers in a filament. Arp2/3 complex also cross-links actin filaments into small bundles and isotropic networks, which are mechanically stiffer than solutions of actin filaments alone. Arp2/3 complex is concentrated at the leading edge of motileAcanthamoeba, and its localization is distinct from that of α-actinin, another filament cross-linking protein. Based on localization and actin filament nucleation and cross-linking activities, we propose a role for Arp2/3 in determining the structure of the actin filament network at the leading edge of motile cells.

scholarly journals Actin Filament Cross-linking by MARCKS

2001 ◽  
Vol 276 (25) ◽  
pp. 22351-22358 ◽  
Author(s):  
Elena G. Yarmola ◽  
Arthur S. Edison ◽  
Robert H. Lenox ◽  
Michael R. Bubb
Keyword(s):  
Actin Filament ◽  
Cross Linking

scholarly journals The F-actin bundler α-actinin Ain1 is tailored for ring assembly and constriction during cytokinesis in fission yeast

2016 ◽  
Vol 27 (11) ◽  
pp. 1821-1833 ◽  
Author(s):  
Yujie Li ◽  
Jenna R. Christensen ◽  
Kaitlin E. Homa ◽  
Glen M. Hocky ◽  
Alice Fok ◽  
...  
Keyword(s):  
Fission Yeast ◽  
Actin Filament ◽  
Actin Filaments ◽  
Biochemical Properties ◽  
Ring Formation ◽  
Cross Linking ◽  
Contractile Ring ◽  
Mixed Polarity ◽  
Dividing Cells

The actomyosin contractile ring is a network of cross-linked actin filaments that facilitates cytokinesis in dividing cells. Contractile ring formation has been well characterized in Schizosaccharomyces pombe, in which the cross-linking protein α-actinin SpAin1 bundles the actin filament network. However, the specific biochemical properties of SpAin1 and whether they are tailored for cytokinesis are not known. Therefore we purified SpAin1 and quantified its ability to dynamically bind and bundle actin filaments in vitro using a combination of bulk sedimentation assays and direct visualization by two-color total internal reflection fluorescence microscopy. We found that, while SpAin1 bundles actin filaments of mixed polarity like other α-actinins, SpAin1 has lower bundling activity and is more dynamic than human α-actinin HsACTN4. To determine whether dynamic bundling is important for cytokinesis in fission yeast, we created the less dynamic bundling mutant SpAin1(R216E). We found that dynamic bundling is critical for cytokinesis, as cells expressing SpAin1(R216E) display disorganized ring material and delays in both ring formation and constriction. Furthermore, computer simulations of initial actin filament elongation and alignment revealed that an intermediate level of cross-linking best facilitates filament alignment. Together our results demonstrate that dynamic bundling by SpAin1 is important for proper contractile ring formation and constriction.

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 Actin filament destruction by osmium tetroxide

1978 ◽  
Vol 77 (3) ◽  
pp. 837-852 ◽  
Author(s):  
P Maupin-Szamier ◽  
TD Pollard
Keyword(s):  
Actin Filament ◽  
Actin Filaments ◽  
Sodium Phosphate ◽  
Osmium Tetroxide ◽  
Time Span ◽  
Cross Linking ◽  
Muscle Actin ◽  
Viscosity Change ◽  
Sodium Phosphate Buffer ◽  
Sulfur Containing

We have studied the destruction of purified muscle actin filaments by osmium tetroxide (OsO4) to develop methods to preserve actin filaments during preparation for electron microscopy. Actin filaments are fragmented during exposure to OsO4. This causes the viscosity of solutions of actin filaments to decrease, ultimately to zero, and provides a convenient quantitative assay to analyze the reaction. The rate of filament destruction is determined by the OsO4 concentration, temperature, buffer type and concentration, and pH. Filament destruction is minimized by treatment with a low concentration of OsO4 in sodium phosphate buffer, pH 6.0, at 0 degrees C. Under these conditions, the viscosity of actin filament solutions is stable and actin filaments retain their straight, unbranched structure, even after dehydration and embedding. Under more severe conditions, the straight actin filaments are converted into what look like the microfilament networks commonly observed in cells fixed with OsO4. Destruction of actin filaments can be inhibited by binding tropomyosin to the actin. Cross-linking the actin molecules within a filament with glutaraldehyde does not prevent their destruction by OsO4. The viscosity decrease requires the continued presence of free OsO4. During the time of the viscosity change, OsO4 is reduced and the sulfur-containing amino acids of actin are oxidized, but little of the osmium is bound to the actin. Over a much longer time span, the actin molecules are split into discrete peptides.

scholarly journals Coordinated waves of actomyosin flow and apical cell constriction immediately after wounding

2013 ◽  
Vol 202 (2) ◽  
pp. 365-379 ◽  
Author(s):  
Marco Antunes ◽  
Telmo Pereira ◽  
João V. Cordeiro ◽  
Luis Almeida ◽  
Antonio Jacinto
Keyword(s):  
Actin Filament ◽  
Transient Receptor Potential ◽  
Apical Cell ◽  
Leading Edge ◽  
Receptor Potential ◽  
Transient Receptor Potential Channel ◽  
Wound Response ◽  
Epithelial Wound Healing ◽  
Cytoskeleton Remodeling ◽  
Transient Receptor

Epithelial wound healing relies on tissue movements and cell shape changes. Our work shows that, immediately after wounding, there was a dramatic cytoskeleton remodeling consisting of a pulse of actomyosin filaments that assembled in cells around the wound edge and flowed from cell to cell toward the margin of the wound. We show that this actomyosin flow was regulated by Diaphanous and ROCK and that it elicited a wave of apical cell constriction that culminated in the formation of the leading edge actomyosin cable, a structure that is essential for wound closure. Calcium signaling played an important role in this process, as its intracellular concentration increased dramatically immediately after wounding, and down-regulation of transient receptor potential channel M, a stress-activated calcium channel, also impaired the actomyosin flow. Lowering the activity of Gelsolin, a known calcium-activated actin filament–severing protein, also impaired the wound response, indicating that cleaving the existing actin filament network is an important part of the cytoskeleton remodeling process.

scholarly journals Nascent adhesions differentially regulate lamellipodium velocity and persistence

2021 ◽  
Author(s):  
Keith R Carney ◽  
Akib M Khan ◽  
Shiela C Samson ◽  
Nikhil Mittal ◽  
Sangyoon J Han ◽  
...  
Keyword(s):  
Cell Migration ◽  
Computational Model ◽  
Actin Filament ◽  
Actin Polymerization ◽  
Leading Edge ◽  
Membrane Tension ◽  
Cell Edge ◽  
Ratchet Mechanism ◽  
Model Predictions ◽  
Clutch Mechanism

Cell migration is essential to physiological and pathological biology. Migration is driven by the motion of a leading edge, in which actin polymerization pushes against the edge and adhesions transmit traction to the substrate while membrane tension increases. How the actin and adhesions synergistically control edge protrusion remains elusive. We addressed this question by developing a computational model in which the Brownian ratchet mechanism governs actin filament polymerization against the membrane and the molecular clutch mechanism governs adhesion to the substrate (BR-MC model). Our model predicted that actin polymerization is the most significant driver of protrusion, as actin had a greater effect on protrusion than adhesion assembly. Increasing the lifetime of nascent adhesions also enhanced velocity, but decreased the protrusion's motional persistence, because filaments maintained against the cell edge ceased polymerizing as membrane tension increased. We confirmed the model predictions with measurement of adhesion lifetime and edge motion in migrating cells. Adhesions with longer lifetime were associated with faster protrusion velocity and shorter persistence. Experimentally increasing adhesion lifetime increased velocity but decreased persistence. We propose a mechanism for actin polymerization-driven, adhesion-dependent protrusion in which balanced nascent adhesion assembly and lifetime generates protrusions with the power and persistence to drive migration.

scholarly journals Unilateral Cleavage Furrows in Multinucleate Cells

Cells ◽  
2020 ◽  
Vol 9 (6) ◽  
pp. 1493 ◽  
Author(s):  
Julia Bindl ◽  
Eszter Sarolta Molnar ◽  
Mary Ecke ◽  
Jana Prassler ◽  
Annette Müller-Taubenberger ◽  
...  
Keyword(s):  
Actin Filament ◽  
Average Velocity ◽  
Electric Pulse ◽  
Myosin Ii ◽  
Cross Linking ◽  
Wild Type ◽  
Initial Direction ◽  
Multinucleate Cells ◽  
Daughter Cells

Multinucleate cells can be produced in Dictyostelium by electric pulse-induced fusion. In these cells, unilateral cleavage furrows are formed at spaces between areas that are controlled by aster microtubules. A peculiarity of unilateral cleavage furrows is their propensity to join laterally with other furrows into rings to form constrictions. This means cytokinesis is biphasic in multinucleate cells, the final abscission of daughter cells being independent of the initial direction of furrow progression. Myosin-II and the actin filament cross-linking protein cortexillin accumulate in unilateral furrows, as they do in the normal cleavage furrows of mononucleate cells. In a myosin-II-null background, multinucleate or mononucleate cells were produced by cultivation either in suspension or on an adhesive substrate. Myosin-II is not essential for cytokinesis either in mononucleate or in multinucleate cells but stabilizes and confines the position of the cleavage furrows. In fused wild-type cells, unilateral furrows ingress with an average velocity of 1.7 µm × min−1, with no appreciable decrease of velocity in the course of ingression. In multinucleate myosin-II-null cells, some of the furrows stop growing, thus leaving space for the extensive broadening of the few remaining furrows.

scholarly journals Isoforms of α-Actinin from Cardiac, Smooth, and Skeletal Muscle Form Polar Arrays of Actin Filaments

2000 ◽  
Vol 149 (3) ◽  
pp. 635-646 ◽  
Author(s):  
Kenneth A. Taylor ◽  
Dianne W. Taylor ◽  
Fred Schachat
Keyword(s):  
Actin Filament ◽  
Actin Filaments ◽  
Polar Filament ◽  
Relative Orientation ◽  
Lipid Monolayer ◽  
Cross Linking ◽  
Internal Diameter ◽  
Vertebrate Muscle ◽  
Filament Bundles ◽  
Positively Charged

We have used a positively charged lipid monolayer to form two-dimensional bundles of F-actin cross-linked by α-actinin to investigate the relative orientation of the actin filaments within them. This method prevents growth of the bundles perpendicular to the monolayer plane, thereby facilitating interpretation of the electron micrographs. Using α-actinin isoforms isolated from the three types of vertebrate muscle, i.e., cardiac, skeletal, and smooth, we have observed almost exclusively cross-linking between polar arrays of filaments, i.e., actin filaments with their plus ends oriented in the same direction. One type of bundle can be classified as an Archimedian spiral consisting of a single actin filament that spirals inward as the filament grows and the bundle is formed. These spirals have a consistent hand and grow to a limiting internal diameter of 0.4–0.7 μm, where the filaments appear to break and spiral formation ceases. These results, using isoforms usually characterized as cross-linkers of bipolar actin filament bundles, suggest that α-actinin is capable of cross-linking actin filaments in any orientation. Formation of specifically bipolar or polar filament arrays cross-linked by α-actinin may require additional factors that either determine the filament orientation or restrict the cross-linking capabilities of α-actinin.

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