Structure of The Z Disk of Sectioned Bee Flight Muscle

1990 ◽  
Vol 48 (1) ◽  
pp. 512-513
Author(s):  
J.F. Deatherage ◽  
N. Cheng
Keyword(s):  
Complex Network ◽  
Actin Filament ◽  
Electron Micrographs ◽  
Central Region ◽  
Actin Filaments ◽  
Flight Muscle ◽  
Opposite Polarity ◽  
Structural Domains ◽  
Thin Sections ◽  
Averaging Technique

Information from oblique thin sections and from 3-D reconstructions of tilted transverse thin sections has been combined to determine the 3-D structure of the honeybee flight muscle Z disk at 7øÅ resolution. The overall symmetry and structure of the Z disk and its relationship to the rest of the myofibril have been determined by tracing filaments and connecting elements on electron images of oblique sections which have been enhanced by a local crystallographic averaging technique .The 3-D structure of the central region of the Z disk of honeybee flight muscle has been determined by crystallographic 3-D reconstruction from electron micrographs of tilted thin sections. The reconstructions show a complex network in which actin filaments terminate and are crosslinked together (Figure 1); a number of structural domains are resolved in the network.The central region of the Z disk contains two sets of overlapping actin filaments of opposite polarity, which originate in the sarcomeres adjacent to the Z disk, and connections between these filaments. The filaments are deflected by the attachment of crosslinks; spacings between filaments change by over 1øøÅ during their passage through the Z disk. Each actin filament is linked by connecting structures to four filaments of opposite polarity and two filaments of the same polarity.

scholarly journals Three-dimensional reconstruction of the Z disk of sectioned bee flight muscle.

1989 ◽  
Vol 108 (5) ◽  
pp. 1761-1774 ◽  
Author(s):  
N Q Cheng ◽  
J F Deatherage
Keyword(s):  
Central Region ◽  
Actin Filaments ◽  
Flight Muscle ◽  
Three Dimensional ◽  
Opposite Polarity ◽  
Dimensional Structure ◽  
Three Dimensional Reconstruction ◽  
Thin Sections ◽  
Dimensional Reconstruction ◽  
Cross Links

The three-dimensional structure of the central region of the Z disk of honeybee flight muscle has been determined to a resolution of 70 A by three-dimensional reconstruction from electron micrographs of tilted thin sections. The reconstructions show a complex assembly in which actin filaments terminate and are cross-linked together; a number of structural domains of this network are resolved in quantitative three-dimensional detail. The central region of the Z disk contains two sets of overlapping actin filaments of opposite polarity, which originate in the sarcomeres adjacent to the Z disk, and connections between these filaments. The filaments are deflected by the attachment of cross-links; spacing between filaments change by greater than 100 A during their passage through the Z disk. Each actin filament is linked by connecting structures to four filaments of opposite polarity and two filaments are of the same polarity. Four types of connecting density domain are observed in association with pairs of filaments of opposite polarity: C1, C2, C3, and C5. Two of these, C3 and C5, are associated with the ends of actin filaments. Another connection, C4, is associated with three filaments of the same polarity; C4 is threefold symmetric.

scholarly journals Arrangement of filaments and cross-links in the bee flight muscle Z disk by image analysis of oblique sections.

1989 ◽  
Vol 108 (5) ◽  
pp. 1775-1782 ◽  
Author(s):  
J F Deatherage ◽  
N Q Cheng ◽  
B Bullard
Keyword(s):  
Actin Filaments ◽  
Flight Muscle ◽  
Three Dimensional ◽  
Thick Filament ◽  
Opposite Polarity ◽  
Dimensional Structure ◽  
Central Plane ◽  
Thin Sections ◽  
Three Dimensional Structure ◽  
Rotation Axes

Information from oblique thin sections and from three-dimensional reconstructions of tilted, transverse thin sections (Cheng, N., and J. F. Deatherage. 1989. J. Cell Biol. 108:1761-1774) has been combined to determine the three-dimensional structure of the honeybee flight muscle Z disk at 70-A resolution. The overall symmetry and structure of the Z disk and its relationship to the rest of the myofibril have been determined by tracing filaments and connecting elements on electron images of oblique sections which have been enhanced by a local crystallographic averaging technique. In the three-dimensional structure, the connecting density between actin filaments can be described as five compact, crystallographically nonequivalent domains. Features C1 and C2 are located on the transverse twofold rotation axes in the central plane of the Z disk. They are associated with the sides of actin filaments of opposite polarity. Features C3, C4, and C5 are present in two symmetry-related sets which are located on opposite sides of the central plane. C3 and C5 are each associated with two filaments of opposite polarity, interacting with the side of one filament and the end of the other filament. C3 and C5 may be involved in stabilizing actin filament ends inside the Z disk. The location of the threefold symmetric connection C4, relative to the thick filament of the adjacent sarcomere, is determined and its possible relationship to the C filament is considered.

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 Actin filament content and organization in unstimulated platelets.

1984 ◽  
Vol 98 (6) ◽  
pp. 1985-1991 ◽  
Author(s):  
J E Fox ◽  
J K Boyles ◽  
C C Reynolds ◽  
D R Phillips
Keyword(s):  
Actin Filament ◽  
Actin Filaments ◽  
Actin Polymerization ◽  
Gel Filtration ◽  
Structural Reorganization ◽  
Filamentous Form ◽  
Thin Sections ◽  
Cell Extracts ◽  
Triton X ◽  
Filament Content

The extent of actin polymerization in unstimulated, discoid platelets was measured by DNase I inhibition assay in Triton X-100 lysates of platelets washed at 37 degrees C by gel filtration, or in Triton X-100 lysates of platelets washed at ambient temperatures by centrifugation in the presence of prostacyclin. About 40% of the actin in the discoid platelets obtained by either method existed as filaments. These filaments could be visualized by electron microscopy of thin sections. Similar results were obtained when the actin filament content of discoid platelets was measured by sedimentation of filaments from Triton X-100 lysates at high g forces (145,000 g for 45 min). However, few of these filaments sedimented at the lower g forces often used to isolate networks of actin filaments from cell extracts. These results indicate that actin filaments in discoid cells are not highly crosslinked. Platelets isolated by centrifugation in the absence of prostacyclin were not discoid, but were instead irregular with one or more pseudopodia. These platelets also contained approximately 40-50% of their actin in a filamentous form; many of these filaments sedimented at low g forces, however, indicating that they were organized into networks. The discoid shape of these centrifuged platelets could be restored by incubating them for 1-3 h at 37 degrees C, which resulted in the reversal of filament organization. High g forces were then required for the sedimentation of the actin. Approximately 80-90% of the actin in platelets washed at 4 degrees C was filamentous; this high actin filament content could be attributed to actin polymerization during the preparation of the platelets at low temperatures. These studies show that platelet activation involves mechanisms for the structural reorganization of existing filaments, in addition to those previously described for mediating actin polymerization.

scholarly journals Formation of actin filament bundles in the ring canals of developing Drosophila follicles.

1996 ◽  
Vol 133 (1) ◽  
pp. 61-74 ◽  
Author(s):  
L G Tilney ◽  
M S Tilney ◽  
G M Guild
Keyword(s):  
Actin Filament ◽  
Actin Filaments ◽  
Actin Binding ◽  
Nurse Cells ◽  
Ring Canal ◽  
Contractile Ring ◽  
Thin Sections ◽  
Development Stages ◽  
Ring Canals ◽  
Filament Bundles

Growing the intracellular bridges that connect nurse cells with each o ther and to the developing oocyte is vital for egg development. These ring canals increase from 0.5 microns in diameter at stage 2 to 10 microns in diameter at stage 11. Thin sections cut horizontally as you would cut a bagel, show that there is a layer of circumferentially oriented actin filaments attached to the plasma membrane at the periphery of each canal. By decoration with subfragment 1 of myosin we find actin filaments of mixed polarities in the ring such as found in the "contractile ring" formed during cytokinesis. In vertical sections through the canal the actin filaments appear as dense dots. At stage 2 there are 82 actin filaments in the ring, by stage 6 there are 717 and by stage 10 there are 726. Taking into account the diameter, this indicates that there is 170 microns of actin filaments/canal at stage 2 (pi x 0.5 microns x 82), 14,000 microns at stage 9 and approximately 23,000 microns at stage 11 or one inch of actin filament! The density of actin filaments remains unchanged throughout development. What is particularly striking is that by stages 4-5, the ring of actin filaments has achieved its maximum thickness, even though the diameter has not yet increased significantly. Thereafter, the diameter increases. Throughout development, stages 2-11, the canal length also increases. Although the density (number of actin filaments/micron2) through a canal remains constant from stage 5 on, the actin filaments appear as a net of interconnected bundles. Further information on this net of bundles comes from studying mutant animals that lack kelch, a protein located in the ring canal that has homology to the actin binding protein, scruin. In this mutant, the actin filaments form normally but individual bundles that comprise the fibers of the net are not bound tightly together. Some bundles enter into the ring canal lumen but do not completely occlude the lumen. all these observations lay the groundwork for our understanding of how a noncontractile ring increases in thickness, diameter, and length during development.

scholarly journals The visualization of actin filament polarity in thin sections. Evidence for the uniform polarity of membrane-associated filaments.

1978 ◽  
Vol 79 (3) ◽  
pp. 846-852 ◽  
Author(s):  
D A Begg ◽  
R Rodewald ◽  
L I Rebhun
Keyword(s):  
Actin Filament ◽  
Actin Filaments ◽  
Intestinal Epithelial ◽  
Improved Method ◽  
Thin Sections ◽  
Myosin Subfragment ◽  
Brush Borders ◽  
Nonmuscle Cells ◽  
Myosin Subfragment 1 ◽  
Uniform Polarity

We have developed an improved method for visualizing actin filament polarity in thin sections. Myosin subfragment-1 (S-1)-decorated actin filaments display a dramatically enhanced arrowhead configuration when fixed in a medium which contains 0.2 % tannic acid. With the exception of brush borders from intestinal epithelial cells, the arrowhead periodicity of decorated filaments in a variety of nonmuscle cells is similar to that in isolated myofibrils. The periodicity of decorated filaments in brush borders is significantly smaller. Actin filaments which attach to membranes display a clear, uniform polarity, with the S-1 arrowheads pointing away from the plasma membrane, while those which comprise the stress fibers of myoblasts and CHO cells have antiparallel polarities. These observations are consistent with a sliding filament mechanism of cell motility.

scholarly journals Actin filaments elongate from their membrane-associated ends

1981 ◽  
Vol 90 (2) ◽  
pp. 485-494 ◽  
Author(s):  
LG Tilney ◽  
EM Bonder ◽  
DJ DeRosier
Keyword(s):  
Plasma Membrane ◽  
Actin Filament ◽  
Actin Filaments ◽  
The Other ◽  
Dense Material ◽  
Thin Sections ◽  
Vacuole Membrane ◽  
Filament Bundles ◽  
Filament Bundle

In limulus sperm an actin filament bundle 55 mum in length extends from the acrosomal vacuole membrane through a canal in the nucleus and then coils in a regular fashion around the base of the nucleus. The bundle expands systematically from 15 filaments near the acrosomal vacuole to 85 filaments at the basal end. Thin sections of sperm fixed during stages in spermatid maturation reveal that the filament bundle begins to assemble on dense material attached to the acrosomal vacuole membrane. In micrographs fo these early stages in maturation, short bundles are seen extending posteriorly from the dense material. The significance is that these short, developing bundles have about 85 filaments, suggesting that the 85-filament end of the bundle is assembled first. By using filament bundles isolated and incubated in vitro with G actin from muscle, we can determine the end "preferred" for addition of actin monomers during polymerization. The end that would be associated with the acrosomal vacuole membrane, a membrane destined to be continuous with the plasma membrane, is preferred about 10 times over the other, thicker end. Decoration of the newly polymerized portions of the filament bundle with subfragment 1 of myosin reveals that the arrowheads point away from the acrosomal vacuole membrane, as is true of other actin filament bundles attached to membranes. From these observations we conclude that the bundle is nucleated from the dense material associated with the acrosomal vacuole and that monomers are added to the membrane-associated end. As monomers are added at the dense material, the thick first-made end of the filament bundle is pushed down through the nucleus where, upon reaching the base of the nucleus, it coils up. Tapering is brought about by the capping of the peripheral filaments in the bundle.

scholarly journals Actin filaments, stereocilia, and hair cells of the bird cochlea. II. Packing of actin filaments in the stereocilia and in the cuticular plate and what happens to the organization when the stereocilia are bent.

1983 ◽  
Vol 96 (3) ◽  
pp. 822-834 ◽  
Author(s):  
L G Tilney ◽  
E H Egelman ◽  
D J DeRosier ◽  
J C Saunder
Keyword(s):  
Actin Filament ◽  
Hair Cells ◽  
Actin Filaments ◽  
Fine Tuning ◽  
Thin Sections ◽  
The Cross ◽  
Diffraction Patterns ◽  
Cross Bridges ◽  
Different Parts ◽  
Filament Bundle

A comparison of hair cells from different parts of the cochlea reveals the same organization of actin filaments; the elements that vary are the length and number of the filaments. Thin sections of stereocilia reveal that the actin filaments are hexagonally packed and from diffraction patterns of these sections we found that the actin filaments are aligned such that the crossover points of adjacent actin filaments are in register. As a result, the cross-bridges that connect adjacent actin filaments are easily seen in longitudinal sections. The cross-bridges appear as regularly spaced bands that are perpendicular to the axis of the stereocilium. Particularly interesting is that, unlike what one might predict, when a stereocilium is bent or displaced, as might occur during stimulation by sound, the actin filaments are not compressed or stretched but slide past one another so that the bridges become tilted relative to the long axis of the actin filament bundle. In the images of bent bundles, the bands of cross-bridges are then tilted off perpendicular to the stereocilium axis. When the stereocilium is bent at its base, all cross-bridges in the stereocilium are affected. Thus, resistance to bending or displacement must be property of the number of bridges present, which in turn is a function of the number of actin filaments present and their respective lengths. Since hair cells in different parts of the cochlea have stereocilia of different, yet predictable lengths and widths, this means that the force needed to displace the stereocilia of hair cells located at different regions of the cochlea will not be the same. This suggests that fine tuning of the hair cells must be a built-in property of the stereocilia. Perhaps its physiological vulnerability may result from changes of stereociliary structure.

The restoration of blurred electron micrographs

1986 ◽  
Vol 44 ◽  
pp. 180-181
Author(s):  
Bridget Carragher ◽  
David A. Bluemke ◽  
Michael J. Potel ◽  
Robert Josephs
Keyword(s):  
Cross Section ◽  
Electron Micrographs ◽  
Relative Motion ◽  
Finite Thickness ◽  
Image Plane ◽  
Helical Axis ◽  
Thin Sections ◽  
Structural Details

We have investigated the feasibility of restoring blurred electron micrographs. Two related problems have been considered; the restoration of images blurred as a result of relative motion between the specimen and the image plane, and the restoration of images which are rotationally blurred about an axis. Micrographs taken while the specimen is drifting result in images which are blurred in the direction of motion. An example of rotational blurring arises in micrographs of thin sections of helical particles viewed in cross section. The twist of the particle within the finite thickness of the section causes the image to appear rotationally blurred about the helical axis. As a result, structural details, particularly at large distances from the helical axis, will be obscured.

scholarly journals Specification of Actin Filament Function and Molecular Composition by Tropomyosin Isoforms

2003 ◽  
Vol 14 (3) ◽  
pp. 1002-1016 ◽  
Author(s):  
Nicole S. Bryce ◽  
Galina Schevzov ◽  
Vicki Ferguson ◽  
Justin M. Percival ◽  
Jim J.-C. Lin ◽  
...  
Keyword(s):  
Cell Size ◽  
Functional Properties ◽  
Actin Filament ◽  
Actin Filaments ◽  
Myosin Ii ◽  
Molecular Composition ◽  
Cellular Migration ◽  
Stress Fibers ◽  
Human Homologue ◽  
Tropomyosin Isoforms

The specific functions of greater than 40 vertebrate nonmuscle tropomyosins (Tms) are poorly understood. In this article we have tested the ability of two Tm isoforms, TmBr3 and the human homologue of Tm5 (hTM5NM1), to regulate actin filament function. We found that these Tms can differentially alter actin filament organization, cell size, and shape. hTm5NM1was able to recruit myosin II into stress fibers, which resulted in decreased lamellipodia and cellular migration. In contrast, TmBr3 transfection induced lamellipodial formation, increased cellular migration, and reduced stress fibers. Based on coimmunoprecipitation and colocalization studies, TmBr3 appeared to be associated with actin-depolymerizing factor/cofilin (ADF)-bound actin filaments. Additionally, the Tms can specifically regulate the incorporation of other Tms into actin filaments, suggesting that selective dimerization may also be involved in the control of actin filament organization. We conclude that Tm isoforms can be used to specify the functional properties and molecular composition of actin filaments and that spatial segregation of isoforms may lead to localized specialization of actin filament function.

Sign in / Sign up

Export Citation Format

Share Document