scholarly journals Active cargo positioning in antiparallel transport networks

2019 ◽  
Author(s):  
Mathieu Richard ◽  
Carles Blanch-Mercader ◽  
Hajer Ennomani ◽  
Wenxiang Cao ◽  
Enrique M. De La Cruz ◽  
...  
Keyword(s):  
Transport Properties ◽  
Molecular Motors ◽  
Actin Filaments ◽  
Actin Polymerization ◽  
Myosin Ii ◽  
Actin Network ◽  
Cargo Transport ◽  
Stochastic Transport ◽  
Mixed Polarity ◽  
Micro Patterns

ABSTRACTCytoskeletal filaments assemble into dense parallel, antiparallel or disordered networks, providing a complex environment for active cargo transport and positioning by molecular motors. The interplay between the network architecture and intrinsic motor properties clearly affects transport properties but remains poorly understood. Here, by using surface micro-patterns of actin polymerization, we investigate stochastic transport properties of colloidal beads in antiparallel networks of overlapping actin filaments. We found that 200-nm beads coated with myosin-Va motors displayed directed movements towards positions where the net polarity of the actin network vanished, accumulating there. The bead distribution was dictated by the spatial profiles of local bead velocity and diffusion coefficient, indicating that a diffusion-drift process was at work. Remarkably, beads coated with heavy mero-myosin-II motors showed a similar behavior. However, although velocity gradients were steeper with myosin II, the much larger bead diffusion observed with this motor resulted in less precise positioning. Our observations are well described by a three-state model, in which active beads locally sense the net polarity of the network by frequently detaching from and reattaching to the filaments. A stochastic sequence of processive runs and diffusive searches results in a biased random walk. The precision of bead positioning is set by the gradient of net actin polarity in the network and by the run length of the cargo in an attached state. Our results unveiled physical rules for cargo transport and positioning in networks of mixed polarity.Significance statementCellular functions rely on small groups of molecular motors to transport their cargoes throughout the cell along polar filaments of the cytoskeleton. Cytoskeletal filaments self-assemble into dense networks comprising intersections and filaments of mixed polarity, challenging directed motor-based transport. Using micro-patterns of actin polymerization in-vitro, we investigated stochastic transport of colloidal beads in antiparallel networks of overlapping actin filaments. We found that beads coated with myosin motors sensed the net polarity of the actin network, resulting in active bead positioning to regions of neutral polarity with a precision depending on the motor type. A theoretical description of our experimental results provides the key physical rules for cargo transport and positioning in filament networks of mixed polarity.

scholarly journals Active cargo positioning in antiparallel transport networks

2019 ◽  
Vol 116 (30) ◽  
pp. 14835-14842 ◽  
Author(s):  
Mathieu Richard ◽  
Carles Blanch-Mercader ◽  
Hajer Ennomani ◽  
Wenxiang Cao ◽  
Enrique M. De La Cruz ◽  
...  
Keyword(s):  
Transport Properties ◽  
Molecular Motors ◽  
Network Architecture ◽  
Actin Polymerization ◽  
Myosin Ii ◽  
Biased Random Walk ◽  
Cargo Transport ◽  
Stochastic Transport ◽  
Mixed Polarity ◽  
Myosin Va

Cytoskeletal filaments assemble into dense parallel, antiparallel, or disordered networks, providing a complex environment for active cargo transport and positioning by molecular motors. The interplay between the network architecture and intrinsic motor properties clearly affects transport properties but remains poorly understood. Here, by using surface micropatterns of actin polymerization, we investigate stochastic transport properties of colloidal beads in antiparallel networks of overlapping actin filaments. We found that 200-nm beads coated with myosin Va motors displayed directed movements toward positions where the net polarity of the actin network vanished, accumulating there. The bead distribution was dictated by the spatial profiles of local bead velocity and diffusion coefficient, indicating that a diffusion-drift process was at work. Remarkably, beads coated with heavy–mero-myosin II motors showed a similar behavior. However, although velocity gradients were steeper with myosin II, the much larger bead diffusion observed with this motor resulted in less precise positioning. Our observations are well described by a 3-state model, in which active beads locally sense the net polarity of the network by frequently detaching from and reattaching to the filaments. A stochastic sequence of processive runs and diffusive searches results in a biased random walk. The precision of bead positioning is set by the gradient of net actin polarity in the network and by the run length of the cargo in an attached state. Our results unveiled physical rules for cargo transport and positioning in networks of mixed polarity.

scholarly journals Actin bundle architecture and mechanics regulate myosin II force generation

2020 ◽  
Author(s):  
Kimberly L. Weirich ◽  
Samantha Stam ◽  
Ed Munro ◽  
Margaret L. Gardel
Keyword(s):  
Actin Filaments ◽  
Myosin Ii ◽  
Force Generation ◽  
Biological Processes ◽  
Actin Bundle ◽  
Force Magnitude ◽  
Cargo Transport ◽  
Mixed Polarity ◽  
Bundle Compliance ◽  
Filament Spacing

AbstractThe actin cytoskeleton is a soft, structural material that underlies biological processes such as cell division, motility, and cargo transport. The cross-linked actin filaments self-organize into a myriad of architectures, from disordered meshworks to ordered bundles, which are hypothesized to control the actomyosin force generation that regulates cell migration, shape, and adhesion. Here, we use fluorescence microscopy and simulations to investigate how actin bundle architectures with varying polarity, spacing, and rigidity impact myosin II dynamics and force generation. Microscopy reveals that mixed polarity bundles formed by rigid cross-linkers support slow, bidirectional myosin II filament motion, punctuated by periods of stalled motion. Simulations reveal that these locations of stalled myosin motion correspond to sustained, high forces in regions of balanced actin filament polarity. By contrast, mixed polarity bundles formed by compliant, large cross-linkers support fast, bidirectional motion with no traps. Simulations indicate that trap duration is directly related to force magnitude, and that the observed increased velocity corresponds to lower forces resulting from both the increased bundle compliance and filament spacing. Our results indicate that the properties of actin structures regulate the dynamics and magnitude of myosin II forces, highlighting the importance of architecture and mechanics in regulating forces in biological materials.

Lymphocyte-Specific Protein 1 Expression in Eukaryotic Cells Reproduces the Morphologic and Motile Abnormality of NAD 47/89 Neutrophils

Blood ◽  
1998 ◽  
Vol 91 (12) ◽  
pp. 4786-4795 ◽  
Author(s):  
Thomas H. Howard ◽  
John Hartwig ◽  
Casey Cunningham
Keyword(s):  
Actin Polymerization ◽  
Cell Function ◽  
Specific Protein ◽  
Polymorphonuclear Neutrophils ◽  
Actin Binding ◽  
Actin Network ◽  
Cell Surfaces ◽  
Actin Bundles ◽  
Mixed Polarity ◽  
Low Levels

Abstract Despite its name, the actin-binding protein lymphocyte-specific protein1 (LSP1) is found in all hematopoetic cells, and yet its role in cell function remains unclear. Recently, LSP1 was identified as the 47-kD protein overexpressed in the polymorphonuclear neutrophils of patients with a rare neutrophil disorder, neutrophil actin dysfunction with abnormalities of 47-kD and 89-kD proteins (NAD 47/89). These neutrophils are immotile, defective in actin polymerization in response to agonists, and display distinctive, fine, “hairlike” F-actin-rich projections on their cell surfaces. We now show that overexpression of LSP1 produces F-actin bundles that are likely responsible for the morphologic and motile abnormalities characteristic of the NAD 47/89 phenotype. Coincident with LSP1 overexpression, cells from each of several different eukaryotic lines, including a highly motile human melanoma line, develop hairlike surface projections that branch distinctively and contain F-actin and LSP1. The hairlike projections are supported at their core by thick actin bundles, composed of actin filaments of mixed polarity, which periodically anastomose to generate a branching structure. The motility of the melanoma cells is inhibited even at low levels of LSP1 expression. Therefore, these studies show that overexpression of LSP1 alone can recreate the morphologic and motile defects seen in NAD 47/89 and suggest that LSP1 is distinct from other known actin binding proteins in its effect on F-actin network structure.

Lymphocyte-Specific Protein 1 Expression in Eukaryotic Cells Reproduces the Morphologic and Motile Abnormality of NAD 47/89 Neutrophils

Blood ◽  
1998 ◽  
Vol 91 (12) ◽  
pp. 4786-4795 ◽  
Author(s):  
Thomas H. Howard ◽  
John Hartwig ◽  
Casey Cunningham
Keyword(s):  
Actin Polymerization ◽  
Cell Function ◽  
Specific Protein ◽  
Polymorphonuclear Neutrophils ◽  
Actin Binding ◽  
Actin Network ◽  
Cell Surfaces ◽  
Actin Bundles ◽  
Mixed Polarity ◽  
Low Levels

Despite its name, the actin-binding protein lymphocyte-specific protein1 (LSP1) is found in all hematopoetic cells, and yet its role in cell function remains unclear. Recently, LSP1 was identified as the 47-kD protein overexpressed in the polymorphonuclear neutrophils of patients with a rare neutrophil disorder, neutrophil actin dysfunction with abnormalities of 47-kD and 89-kD proteins (NAD 47/89). These neutrophils are immotile, defective in actin polymerization in response to agonists, and display distinctive, fine, “hairlike” F-actin-rich projections on their cell surfaces. We now show that overexpression of LSP1 produces F-actin bundles that are likely responsible for the morphologic and motile abnormalities characteristic of the NAD 47/89 phenotype. Coincident with LSP1 overexpression, cells from each of several different eukaryotic lines, including a highly motile human melanoma line, develop hairlike surface projections that branch distinctively and contain F-actin and LSP1. The hairlike projections are supported at their core by thick actin bundles, composed of actin filaments of mixed polarity, which periodically anastomose to generate a branching structure. The motility of the melanoma cells is inhibited even at low levels of LSP1 expression. Therefore, these studies show that overexpression of LSP1 alone can recreate the morphologic and motile defects seen in NAD 47/89 and suggest that LSP1 is distinct from other known actin binding proteins in its effect on F-actin network structure.

scholarly journals Analysis of the Actin–Myosin II System in Fish Epidermal Keratocytes: Mechanism of Cell Body Translocation

1997 ◽  
Vol 139 (2) ◽  
pp. 397-415 ◽  
Author(s):  
Tatyana M. Svitkina ◽  
Alexander B. Verkhovsky ◽  
Kyle M. McQuade ◽  
Gary G. Borisy
Keyword(s):  
Cell Body ◽  
Actin Filaments ◽  
Actin Polymerization ◽  
Myosin Ii ◽  
Leading Edge ◽  
Time Lapse ◽  
Supramolecular Organization ◽  
Retrograde Flow ◽  
Body Boundary ◽  
Filament Bundles

While the protrusive event of cell locomotion is thought to be driven by actin polymerization, the mechanism of forward translocation of the cell body is unclear. To elucidate the mechanism of cell body translocation, we analyzed the supramolecular organization of the actin–myosin II system and the dynamics of myosin II in fish epidermal keratocytes. In lamellipodia, long actin filaments formed dense networks with numerous free ends in a brushlike manner near the leading edge. Shorter actin filaments often formed T junctions with longer filaments in the brushlike area, suggesting that new filaments could be nucleated at sides of preexisting filaments or linked to them immediately after nucleation. The polarity of actin filaments was almost uniform, with barbed ends forward throughout most of the lamellipodia but mixed in arc-shaped filament bundles at the lamellipodial/cell body boundary. Myosin II formed discrete clusters of bipolar minifilaments in lamellipodia that increased in size and density towards the cell body boundary and colocalized with actin in boundary bundles. Time-lapse observation demonstrated that myosin clusters appeared in the lamellipodia and remained stationary with respect to the substratum in locomoting cells, but they exhibited retrograde flow in cells tethered in epithelioid colonies. Consequently, both in locomoting and stationary cells, myosin clusters approached the cell body boundary, where they became compressed and aligned, resulting in the formation of boundary bundles. In locomoting cells, the compression was associated with forward displacement of myosin features. These data are not consistent with either sarcomeric or polarized transport mechanisms of cell body translocation. We propose that the forward translocation of the cell body and retrograde flow in the lamellipodia are both driven by contraction of an actin–myosin network in the lamellipodial/cell body transition zone.

Polarity sorting of actin filaments in cytochalasin-treated fibroblasts

1997 ◽  
Vol 110 (15) ◽  
pp. 1693-1704 ◽  
Author(s):  
A.B. Verkhovsky ◽  
T.M. Svitkina ◽  
G.G. Borisy
Keyword(s):  
Actin Filament ◽  
Actin Filaments ◽  
Myosin Ii ◽  
Dynamic Network ◽  
Muscle Cells ◽  
Immunogold Labelling ◽  
Cultured Fibroblasts ◽  
Myosin S1 ◽  
Mixed Polarity ◽  
Myosin Interaction

The polarity of actin filaments is fundamental for the subcellular mechanics of actin-myosin interaction; however, little is known about how actin filaments are oriented with respect to myosin in non-muscle cells and how actin polarity organization is established and maintained. Here we approach these questions by investigating changes in the organization and polarity of actin relative to myosin II during actin filament translocation. Actin and myosin II reorganization was followed both kinetically, using microinjected fluorescent analogs of actin and myosin, and ultrastructurally, using myosin S1 decoration and immunogold labelling, in cultured fibroblasts that were induced to contract by treatment with cytochalasin D. We observed rapid (within 15 minutes) formation of ordered actin filament arrays: short tapered bundles and aster-like assemblies, in which filaments had uniform polarity with their barbed ends oriented toward the aggregate of myosin II at the base of a bundle or in the center of an aster. The resulting asters further interacted with each other and aggregated into bigger asters. The arrangement of actin in asters was in sharp contrast to the mixed polarity of actin filaments relative to myosin in non-treated cells. At the edge of the cell, actin filaments became oriented with their barbed ends toward the cell center; that is, the orientation was opposite to what was observed at the edge of nontreated cells. This rearrangement is indicative of relative translocation of actin and myosin II and of the ability of myosin II to sort actin filaments with respect to their polarity during translocation. The results suggest that the myosin II-actin system of non-muscle cells is organized as a dynamic network where actin filament arrangement is defined in the course of its interaction with myosin II.

scholarly journals Actin turnover maintains actin filament homeostasis during cytokinetic ring contraction

2017 ◽  
Vol 216 (9) ◽  
pp. 2657-2667 ◽  
Author(s):  
Ting Gang Chew ◽  
Junqi Huang ◽  
Saravanan Palani ◽  
Ruth Sommese ◽  
Anton Kamnev ◽  
...  
Keyword(s):  
Actin Filament ◽  
Actin Filaments ◽  
Actin Polymerization ◽  
Myosin Ii ◽  
Contractile Ring ◽  
Ring Contraction ◽  
Actin Turnover ◽  
Exogenous Addition ◽  
Turn Over

Cytokinesis in many eukaryotes involves a tension-generating actomyosin-based contractile ring. Many components of actomyosin rings turn over during contraction, although the significance of this turnover has remained enigmatic. Here, using Schizosaccharomyces japonicus, we investigate the role of turnover of actin and myosin II in its contraction. Actomyosin ring components self-organize into ∼1-µm-spaced clusters instead of undergoing full-ring contraction in the absence of continuous actin polymerization. This effect is reversed when actin filaments are stabilized. We tested the idea that the function of turnover is to ensure actin filament homeostasis in a synthetic system, in which we abolished turnover by fixing rings in cell ghosts with formaldehyde. We found that these rings contracted fully upon exogenous addition of a vertebrate myosin. We conclude that actin turnover is required to maintain actin filament homeostasis during ring contraction and that the requirement for turnover can be bypassed if homeostasis is achieved artificially.

scholarly journals Myosin-driven fragmentation of actin filaments triggers contraction of a disordered actin network

2018 ◽  
Author(s):  
Kyohei Matsuda ◽  
Takuya Kobayashi ◽  
Mitsuhiro Sugawa ◽  
Yurika Koiso ◽  
Yoko Y. Toyoshima ◽  
...  
Keyword(s):  
Molecular Mechanism ◽  
Actin Filaments ◽  
Atp Hydrolysis ◽  
Myosin Ii ◽  
Network Connectivity ◽  
Experimental System ◽  
Actin Network ◽  
Atp Concentration ◽  
Time Required

AbstractThe dynamic cytoskeletal network is responsible for cell shape changes and cell division. The actin-based motor protein myosin II drives the remodeling of a highly disordered actin-based network and enables the network to perform mechanical work such as contraction, migration and adhesion. Myosin II forms bipolar filaments that self-associate via their tail domains. Such myosin minifilaments generate both extensile and compressive forces that pull and push actin filaments, depending on the relative position of myosin and actin filaments in the network. However, it remains unclear how the mechanical properties of myosin II that rely on the energy of ATP hydrolysis spontaneously contract the disordered actin network. Here, we used a minimal in vitro reconstituted experimental system consisting of actin, myosin, and a cross-linking protein, to gain insights into the molecular mechanism by which myosin minifilaments organize disordered actin networks into contractile states. We found that contracted cluster size and time required for the onset of network contraction decreased as ATP concentration decreased. Contraction velocity was negatively correlated with ATP concentrations. Reduction of ATP concentration caused fragmentation of actin filaments by myosin minifilament. We also found that gelsolin, a Ca2+-regulated actin filament-severing protein, induced contraction of a mechanically stable network, implying that fragmentations of actin filaments in the network weaken the intra-network connectivity and trigger contraction. Our findings reveal that the disordered actin network contraction can be controlled by fragmentation of actin filaments, highlighting the molecular mechanism underlying the myosin motor-severing activities, other than the sliding tensile and compressive stress in the disordered actin network.

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 Discrete mechanical model of lamellipodial actin network implements molecular clutch mechanism and generates arcs and microspikes

2021 ◽  
Vol 17 (10) ◽  
pp. e1009506
Author(s):  
David M. Rutkowski ◽  
Dimitrios Vavylonis
Keyword(s):  
Actin Filaments ◽  
Actin Polymerization ◽  
Focal Adhesions ◽  
Leading Edge ◽  
Flow Speed ◽  
Viscous Drag ◽  
Stress Profile ◽  
Retrograde Flow ◽  
Actin Network ◽  
Clutch Mechanism

Mechanical forces, actin filament turnover, and adhesion to the extracellular environment regulate lamellipodial protrusions. Computational and mathematical models at the continuum level have been used to investigate the molecular clutch mechanism, calculating the stress profile through the lamellipodium and around focal adhesions. However, the forces and deformations of individual actin filaments have not been considered while interactions between actin networks and actin bundles is not easily accounted with such methods. We develop a filament-level model of a lamellipodial actin network undergoing retrograde flow using 3D Brownian dynamics. Retrograde flow is promoted in simulations by pushing forces from the leading edge (due to actin polymerization), pulling forces (due to molecular motors), and opposed by viscous drag in cytoplasm and focal adhesions. Simulated networks have densities similar to measurements in prior electron micrographs. Connectivity between individual actin segments is maintained by permanent and dynamic crosslinkers. Remodeling of the network occurs via the addition of single actin filaments near the leading edge and via filament bond severing. We investigated how several parameters affect the stress distribution, network deformation and retrograde flow speed. The model captures the decrease in retrograde flow upon increase of focal adhesion strength. The stress profile changes from compression to extension across the leading edge, with regions of filament bending around focal adhesions. The model reproduces the observed reduction in retrograde flow speed upon exposure to cytochalasin D, which halts actin polymerization. Changes in crosslinker concentration and dynamics, as well as in the orientation pattern of newly added filaments demonstrate the model’s ability to generate bundles of filaments perpendicular (actin arcs) or parallel (microspikes) to the protruding direction.

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