scholarly journals Myosin II filament assemblies in the active lamella of fibroblasts: their morphogenesis and role in the formation of actin filament bundles.

1995 ◽  
Vol 131 (4) ◽  
pp. 989-1002 ◽  
Author(s):  
A B Verkhovsky ◽  
T M Svitkina ◽  
G G Borisy
Keyword(s):  
Electron Microscopy ◽  
Actin Filament ◽  
Mammalian Cells ◽  
Myosin Ii ◽  
Myosin Filament ◽  
Actin Bundles ◽  
Fluorescence And Electron Microscopy ◽  
Myosin Filaments ◽  
Filament Bundles ◽  
Filament Network

The morphogenesis of myosin II structures in active lamella undergoing net protrusion was analyzed by correlative fluorescence and electron microscopy. In rat embryo fibroblasts (REF 52) microinjected with tetramethylrhodamine-myosin II, nascent myosin spots formed close to the active edge during periods of retraction and then elongated into wavy ribbons of uniform width. The spots and ribbons initially behaved as distinct structural entities but subsequently aligned with each other in a sarcomeric-like pattern. Electron microscopy established that the spots and ribbons consisted of bipolar minifilaments associated with each other at their head-containing ends and arranged in a single row in an "open" zig-zag conformation or as a "closed" parallel stack. Ribbons also contacted each other in a nonsarcomeric, network-like arrangement as described previously (Verkhovsky and Borisy, 1993. J. Cell Biol. 123:637-652). Myosin ribbons were particularly pronounced in REF 52 cells, but small ribbons and networks were found also in a range of other mammalian cells. At the edge of the cell, individual spots and open ribbons were associated with relatively disordered actin filaments. Further from the edge, myosin filament alignment increased in parallel with the development of actin bundles. In actin bundles, the actin cross-linking protein, alpha-actinin, was excluded from sites of myosin localization but concentrated in paired sites flanking each myosin ribbon, suggesting that myosin filament association may initiate a pathway for the formation of actin filament bundles. We propose that zig-zag assemblies of myosin II filaments induce the formation of actin bundles by pulling on an actin filament network and that co-alignment of actin and myosin filaments proceeds via folding of myosin II filament assemblies in an accordion-like fashion.

scholarly journals Non-sarcomeric mode of myosin II organization in the fibroblast lamellum.

1993 ◽  
Vol 123 (3) ◽  
pp. 637-652 ◽  
Author(s):  
A B Verkhovsky ◽  
G G Borisy
Keyword(s):  
Fluorescence Microscopy ◽  
Myosin Ii ◽  
Distribution Patterns ◽  
Myosin Filament ◽  
Fluorescence And Electron Microscopy ◽  
Living State ◽  
Lamellar Region ◽  
And Control ◽  
Muscle Myosin ◽  
Filament Network

The organization of myosin in the fibroblast lamellum was studied by correlative fluorescence and electron microscopy after a novel procedure to reveal its underlying morphology. An X-rhodamine analog of conventional smooth muscle myosin (myosin II) that colocalized after microinjection with endogenous myosin was used to trace myosin distribution in living fibroblasts. Then, the same cells were examined by EM of platinum replicas. To visualize the structural arrangement of myosin, other cytoskeletal fibrillar structures had to be removed: microtubules were depolymerized by nocodazole treatment of the living cells before injection of myosin; continued nocodazole treatment also induced the intermediate filaments to concentrate near the nucleus, thus removing them from the lamellar region; actin filaments were removed after lysis of the cells by incubation of the cytoskeletons with recombinant gelsolin. Possible changes in myosin organization caused by this treatment were examined by fluorescence microscopy. No significant differences in myosin distribution patterns between nocodazole-treated and control cells were observed. Cell lysis and depletion of actin also did not induce reorganization of myosin as was shown by direct comparison of myosin distribution in the same cells in the living state and after gelsolin treatment. EM of the well-spread, peripheral regions of actin-depleted cytoskeletons revealed a network of bipolar myosin mini-filaments, contracting each other at their terminal, globular regions. The morphology of this network corresponded well to the myosin distribution observed by fluorescence microscopy. A novel mechanism of cell contraction by folding of the myosin filament network is proposed.

scholarly journals Molecular Architecture of Synaptic Actin Cytoskeleton in Hippocampal Neurons Reveals a Mechanism of Dendritic Spine Morphogenesis

2010 ◽  
Vol 21 (1) ◽  
pp. 165-176 ◽  
Author(s):  
Farida Korobova ◽  
Tatyana Svitkina
Keyword(s):  
Electron Microscopy ◽  
Actin Cytoskeleton ◽  
Actin Filament ◽  
Dendritic Spines ◽  
Dendritic Spine ◽  
Myosin Ii ◽  
Capping Protein ◽  
Dominant Feature ◽  
Presynaptic Boutons ◽  
Spine Morphogenesis

Excitatory synapses in the brain play key roles in learning and memory. The formation and functions of postsynaptic mushroom-shaped structures, dendritic spines, and possibly of presynaptic terminals, rely on actin cytoskeleton remodeling. However, the cytoskeletal architecture of synapses remains unknown hindering the understanding of synapse morphogenesis. Using platinum replica electron microscopy, we characterized the cytoskeletal organization and molecular composition of dendritic spines, their precursors, dendritic filopodia, and presynaptic boutons. A branched actin filament network containing Arp2/3 complex and capping protein was a dominant feature of spine heads and presynaptic boutons. Surprisingly, the spine necks and bases, as well as dendritic filopodia, also contained a network, rather than a bundle, of branched and linear actin filaments that was immunopositive for Arp2/3 complex, capping protein, and myosin II, but not fascin. Thus, a tight actin filament bundle is not necessary for structural support of elongated filopodia-like protrusions. Dynamically, dendritic filopodia emerged from densities in the dendritic shaft, which by electron microscopy contained branched actin network associated with dendritic microtubules. We propose that dendritic spine morphogenesis begins from an actin patch elongating into a dendritic filopodium, which tip subsequently expands via Arp2/3 complex-dependent nucleation and which length is modulated by myosin II-dependent contractility.

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 Filament evanescence of myosin II and smooth muscle function

2021 ◽  
Vol 153 (3) ◽  
Author(s):  
Lu Wang ◽  
Pasquale Chitano ◽  
Chun Y. Seow
Keyword(s):  
Smooth Muscle ◽  
Muscle Function ◽  
Molecular Mechanisms ◽  
Striated Muscle ◽  
Myosin Ii ◽  
Length Distribution ◽  
Myosin Filament ◽  
New Paradigm ◽  
Smooth Muscle Function ◽  
Myosin Filaments

Smooth muscle is an integral part of hollow organs. Many of them are constantly subjected to mechanical forces that alter organ shape and modify the properties of smooth muscle. To understand the molecular mechanisms underlying smooth muscle function in its dynamic mechanical environment, a new paradigm has emerged that depicts evanescence of myosin filaments as a key mechanism for the muscle’s adaptation to external forces in order to maintain optimal contractility. Unlike the bipolar myosin filaments of striated muscle, the side-polar filaments of smooth muscle appear to be less stable, capable of changing their lengths through polymerization and depolymerization (i.e., evanescence). In this review, we summarize accumulated knowledge on the structure and mechanism of filament formation of myosin II and on the influence of ionic strength, pH, ATP, myosin regulatory light chain phosphorylation, and mechanical perturbation on myosin filament stability. We discuss the scenario of intracellular pools of monomeric and filamentous myosin, length distribution of myosin filaments, and the regulatory mechanisms of filament lability in contraction and relaxation of smooth muscle. Based on recent findings, we suggest that filament evanescence is one of the fundamental mechanisms underlying smooth muscle’s ability to adapt to the external environment and maintain optimal function. Finally, we briefly discuss how increased ROCK protein expression in asthma may lead to altered myosin filament stability, which may explain the lack of deep-inspiration–induced bronchodilation and bronchoprotection in asthma.

scholarly journals Mechanical model of muscle contraction 2. Kinematic and dynamic aspects of a myosin II head during the working stroke

2019 ◽  
Author(s):  
S. Louvet
Keyword(s):  
Actin Filament ◽  
Myosin Head ◽  
Myosin Ii ◽  
Tangential Force ◽  
Longitudinal Axis ◽  
Myosin Filament ◽  
Analytical Relationship ◽  
Shortening Velocity ◽  
Fixed Plane ◽  
Algorithmic Optimization

AbstractThe condition of a myosin II head during which force and movement are generated is commonly referred to as Working Stroke (WS). During the WS, the myosin head is mechanically modelled by 3 two by two articulated segments, the motor domain (S1a) strongly fixed to an actin molecule, the lever (S1b) on which a motor moment is exerted, and the rod (S2) pulling the myosin filament (Mfil). When the half-sarcomere (hs) is shortened or lengthened by a few nanometers, it is assumed that the lever of a myosin head in WS state moves in a fixed plane including the longitudinal axis of the actin filament (Afil). As a result, the 5 rigid segments, i.e. Afil, S1a, S1b, S2 and Mfil, follow deterministic and configurable trajectories. The orientation of S1b in the fixed plane is characterized by the angle θ. After deriving the geometric equations singularizing the WS state, we obtain an analytical relationship between the hs shortening velocity (u) and the angular velocity of the lever . The principles of classical mechanics applied to the 3 solids, S1a, S1b and S2, lead to a relationship between the motor moment exerted on the lever (MB) and the tangential force dragging the actin filament (TA). We distinguish θup and θdown, the two boundaries framing the angle θ during the WS, relating to up and down conformations. With the usual data assigned to the cross-bridge elements, a linearization procedure of the relationships between u and , on the one hand, and between MB and TA, on the other hand, is performed. This algorithmic optimization leads to theoretical values of θup and θdown equal to +28° (−28°) and −42° (+42°) respectively with a variability of ±5° in a hs on the right (left), data in accordance with the commonly accepted experimental values for vertebrate muscle fibers.

scholarly journals Unidirectional sliding of myosin filaments along the bundle of F-actin filaments spontaneously formed during superprecipitation.

1985 ◽  
Vol 101 (6) ◽  
pp. 2335-2344 ◽  
Author(s):  
S Higashi-Fujime
Keyword(s):  
Actin Filament ◽  
Actin Filaments ◽  
Room Temperature ◽  
The Other ◽  
Reverse Direction ◽  
Myosin Filament ◽  
Bipolar Structure ◽  
Myosin Filaments ◽  
Direction Of Movement ◽  
Cold Spring

I reported previously (Higashi-Fujime, S., 1982, Cold Spring Harbor Symp. Quant. Biol., 46:69-75) that active movements of fibrils composed of F-actin and myosin filaments occurred after superprecipitation in the presence of ATP at low ionic strengths. When the concentration of MgCl2 in the medium used in the above experiment was raised to 20-26 mM, bundles of F-actin filaments, in addition to large precipitates, were formed spontaneously both during and after superprecipitation. Along these bundles, many myosin filaments were observed to slide unidirectionally and successively through the bundle, from one end to the other. The sliding of myosin filaments continued for approximately 1 h at room temperature at a mean rate of 6.0 micron/s, as long as ATP remained in the medium. By electron microscopy, it was found that most F-actin filaments decorated with heavy meromyosin pointed to the same direction in the bundle. Myosin filaments moved actively not only along the F-actin bundle but also in the medium. Such movement probably occurred along F-actin filaments that did not form the bundle but were dispersed in the medium, although dispersed F-actin filaments were not visible under the microscope. In this case, myosin filament could have moved in a reverse direction, changing from one F-actin filament to the other. These results suggested that the direction of movement of myosin filament, which has a bipolar structure and the potentiality to move in both directions, was determined by the polarity of F-actin filament in action.

scholarly journals HSPB7 is indispensable for heart development by modulating actin filament assembly

2017 ◽  
Vol 114 (45) ◽  
pp. 11956-11961 ◽  
Author(s):  
Tongbin Wu ◽  
Yongxin Mu ◽  
Julius Bogomolovas ◽  
Xi Fang ◽  
Jennifer Veevers ◽  
...  
Keyword(s):  
Heat Shock ◽  
Heat Shock Protein ◽  
Actin Filament ◽  
Thin Filament ◽  
Actin Polymerization ◽  
Small Heat Shock Protein ◽  
Embryonic Lethality ◽  
Filament Length ◽  
Actin Bundles ◽  
Filament Bundles

Small heat shock protein HSPB7 is highly expressed in the heart. Several mutations within HSPB7 are associated with dilated cardiomyopathy and heart failure in human patients. However, the precise role of HSPB7 in the heart is still unclear. In this study, we generated global as well as cardiac-specific HSPB7 KO mouse models and found that loss of HSPB7 globally or specifically in cardiomyocytes resulted in embryonic lethality before embryonic day 12.5. Using biochemical and cell culture assays, we identified HSPB7 as an actin filament length regulator that repressed actin polymerization by binding to monomeric actin. Consistent with HSPB7’s inhibitory effects on actin polymerization, HSPB7 KO mice had longer actin/thin filaments and developed abnormal actin filament bundles within sarcomeres that interconnected Z lines and were cross-linked by α-actinin. In addition, loss of HSPB7 resulted in up-regulation of Lmod2 expression and mislocalization of Tmod1. Furthermore, crossing HSPB7 null mice into an Lmod2 null background rescued the elongated thin filament phenotype of HSPB7 KOs, but double KO mice still exhibited formation of abnormal actin bundles and early embryonic lethality. These in vivo findings indicated that abnormal actin bundles, not elongated thin filament length, were the cause of embryonic lethality in HSPB7 KOs. Our findings showed an unsuspected and critical role for a specific small heat shock protein in directly modulating actin thin filament length in cardiac muscle by binding monomeric actin and limiting its availability for polymerization.

scholarly journals Human platelet myosin. II. In vitro assembly and structure of myosin filaments.

1975 ◽  
Vol 67 (1) ◽  
pp. 72-92 ◽  
Author(s):  
R Niederman ◽  
T D Pollard
Keyword(s):  
Electron Microscopy ◽  
Ionic Strength ◽  
Thin Section ◽  
Human Platelet ◽  
Myosin Ii ◽  
Myosin Molecule ◽  
Myosin Filaments ◽  
In Vitro Assembly ◽  
Myosin Rod

We have used electron microscopy and solubility measurements to investigate the assembly and structure of purified human platelet myosin and myosin rod into filaments. In buffers with ionic strengths of less than 0.3 M, platelet myosin forms filaments which are remarkable for their small size, being only 320 nm long and 10-11 nm wide in the center of the bare zone. The dimensions of these filaments are not affected greatly by variation of the pH between 7 and 8, variation of the ionic strength between 0.05 and 0.2 M, the presence or absence of 1 mM Mg++ or ATP, or variation of the myosin concentration between 0.05 and 0.7 mg/ml. In 1 mM Ca++ and at pH 6.5 the filaments grow slightly larger. More than 90% of purified platelet myosin molecules assemble into filaments in 0.1 M KC1 at pH 7. Purified preparations of the tail fragment of platelet myosin also form filaments. These filaments are slightly larger than myosin filaments formed under the same conditions, indicating that the size of the myosin filaments may be influenced by some interaction between the head and tail portions of myosin molecules. Calculations based on the size and shape of the myosin filaments, the dimensions of the myosin molecule and analysis of the bare zone reveal that the synthetic platelet myosin filaments consists of 28 myosin molecules arranged in a bipolar array with the heads of two myosin molecules projecting from the backbone of the filament at 14-15 nm intervals. The heads appear to be loosely attached to the backbone by a flexible portion of the myosin tail. Given the concentration of myosin in platelets and the number of myosin molecules per filament, very few of these thin myosin filaments should be present in a thin section of a platelet, even if all of the myosin molecules are aggregated into filaments.

scholarly journals Non-canonical apical constriction shapes emergent matrices in C. elegans

2018 ◽  
Author(s):  
Sophie S. Katz ◽  
Chloe Maybrun ◽  
Hannah M. Maul-Newby ◽  
Alison R. Frand
Keyword(s):  
Actin Filament ◽  
Larval Stage ◽  
Body Wall ◽  
Matrix Remodeling ◽  
Apical Constriction ◽  
Actin Bundles ◽  
C Elegans ◽  
Filament Bundles ◽  
Body Wall Muscles

ABSTRACTSpecialized epithelia produce apical matrices with distinctive topographies by enigmatic mechanisms. Here, we describe a holistic mechanism that integrates cortical actomyosin dynamics with apical matrix remodeling to pattern C. elegans cuticles. Therein, axial AFBs appear near the surface of lateral epidermal syncytia during an interval of transverse apical constriction (AC). AC gives rise to three temporary semi-circular cellular protrusions beneath a provisional matrix (sheath). In turn, sheath components pattern durable ridges along the midline of adult cuticles (alae). We propose that forces generated by AC are relayed via the sheath to sculpt the the acellular adult cuticle manifest several hours later. Furthermore, we provide evidence that circumferential actin filament bundles (CFBs) near the surface of the adjacent syncytia (hyp7) are largely dispensable for the propagation of annular cuticle structures from one larval stage to the next. Rather, the temporary CFBs extend from actin bundles overlying body wall muscles, which are situated between Ce. hemidesmosomes. Similar mechanisms may contribute to the morphogenesis of integumentary organs in higher metazoans.

scholarly journals Ordering of myosin II filaments driven by mechanical forces: experiments and theory

2018 ◽  
Vol 373 (1747) ◽  
pp. 20170114 ◽  
Author(s):  
Kinjal Dasbiswas ◽  
Shiqiong Hu ◽  
Frank Schnorrer ◽  
Samuel A. Safran ◽  
Alexander D. Bershadsky
Keyword(s):  
Actin Cytoskeleton ◽  
Actin Filament ◽  
Cell Biology ◽  
Striated Muscle ◽  
Myosin Ii ◽  
Muscle Cells ◽  
Self Organization ◽  
The Matrix ◽  
Filament Bundles ◽  
And Function

Myosin II filaments form ordered superstructures in both cross-striated muscle and non-muscle cells. In cross-striated muscle, myosin II (thick) filaments, actin (thin) filaments and elastic titin filaments comprise the stereotypical contractile units of muscles called sarcomeres. Linear chains of sarcomeres, called myofibrils, are aligned laterally in registry to form cross-striated muscle cells. The experimentally observed dependence of the registered organization of myofibrils on extracellular matrix elasticity has been proposed to arise from the interactions of sarcomeric contractile elements (considered as force dipoles) through the matrix. Non-muscle cells form small bipolar filaments built of less than 30 myosin II molecules. These filaments are associated in registry forming superstructures (‘stacks’) orthogonal to actin filament bundles. Formation of myosin II filament stacks requires the myosin II ATPase activity and function of the actin filament crosslinking, polymerizing and depolymerizing proteins. We propose that the myosin II filaments embedded into elastic, intervening actin network (IVN) function as force dipoles that interact attractively through the IVN. This is in analogy with the theoretical picture developed for myofibrils where the elastic medium is now the actin cytoskeleton itself. Myosin stack formation in non-muscle cells provides a novel mechanism for the self-organization of the actin cytoskeleton at the level of the entire cell. This article is part of the theme issue ‘Self-organization in cell biology’.

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