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.

scholarly journals The actin filament content of hair cells of the bird cochlea is nearly constant even though the length, width, and number of stereocilia vary depending on the hair cell location.

1988 ◽  
Vol 107 (6) ◽  
pp. 2563-2574 ◽  
Author(s):  
L G Tilney ◽  
M S Tilney
Keyword(s):  
Hair Cell ◽  
Actin Filament ◽  
Cross Sections ◽  
Hair Cells ◽  
Actin Filaments ◽  
Membrane Surface ◽  
Scanning Electron Micrographs ◽  
Length Width ◽  
Filament Content ◽  
Filament Bundle

By direct counts off scanning electron micrographs, we determined the number of stereocilia per hair cell of the chicken cochlea as a function of the position of the hair cell on the cochlea. Micrographs of thin cross sections of stereociliary bundles located at known positions on the cochlea were enlarged and the total number of actin filaments per stereocilium was counted and recorded. By comparing the counts of filament number with measurements of actin filament bundle width of the same stereocilium, we were able to relate actin filament bundle width to filament number with an error margin (r2) of 16%. Combining this data with data already published or in the process of publication from our laboratory on the length and width of stereocilia, we were able to calculate the total length of actin filaments present in stereociliary bundles of hair cells located at a variety of positions on the cochlea. We found that stereociliary bundles of hair cells contain 80,000-98,000 micron of actin filament, i.e., the concentration of actin is constant in all hair cells with a range of values that is less than our error in measurement and/or biological variation, the greatest variation being in relating the diameters of the stereocilia to filament number. We also calculated the membrane surface needed to cover the stereocilia of hair cells located throughout the cochlea. The values (172-192 micron 2) are also constant. The implications of our observation that the total amount of actin is constant even though the length, width, and number of stereocilia per hair cell vary are discussed.

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 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 THE DOUBLE ARRAY OF FILAMENTS IN CROSS-STRIATED MUSCLE

1957 ◽  
Vol 3 (5) ◽  
pp. 631-648 ◽  
Author(s):  
H. E. Huxley
Keyword(s):  
Striated Muscle ◽  
The Other ◽  
Thin Sections ◽  
Alternative Models ◽  
Double Array ◽  
The Cross ◽  
Cross Bridges

The conditions under which one might expect to see the secondary filaments (if they exist) in longitudinal sections of striated muscle, are discussed. It is shown that these conditions were not satisfied in previously published works for the sections were too thick. When suitably thin sections are examined, the secondary filaments can be seen perfectly easily. It is also possible to see clearly other details of the structure, notably the cross-bridges between primary and secondary filaments, and the tapering of the primary filaments at their ends. The arrangement of the filaments and the changes associated with contraction and with stretch are identical to those already deduced from previous observations and described in terms of the interdigitating filament model in previous papers. There are therefore excellent grounds for believing that this model is correct. The alternative models which have been proposed appear to be incompatible both with the present observations and with much of the other available evidence.

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 Reassociation of microvillar core proteins: making a microvillar core in vitro.

1989 ◽  
Vol 108 (2) ◽  
pp. 495-502 ◽  
Author(s):  
L M Coluccio ◽  
A Bretscher
Keyword(s):  
Actin Filaments ◽  
Direct Proof ◽  
Intestinal Epithelia ◽  
The Core ◽  
Cross Bridge ◽  
Core Proteins ◽  
The Cross ◽  
Cross Bridges

Intestinal epithelia have a brush border membrane of numerous microvilli each comprised of a cross-linked core bundle of 15-20 actin filaments attached to the surrounding membrane by lateral cross-bridges; the cross-bridges are tilted with respect to the core bundle. Isolated microvillar cores contain actin (42 kD) and three other major proteins: fimbrin (68 kD), villin (95 kD), and the 110K-calmodulin complex. The addition of ATP to detergent-treated isolated microvillar cores has previously been shown to result in loss of the lateral cross-bridges and a corresponding decrease in the amount of the 110-kD polypeptide and calmodulin associated with the core bundle. This provided the first evidence to suggest that these lateral cross-bridges to the membrane are comprised at least in part by a 110-kD polypeptide complexed with calmodulin. We now demonstrate that purified 110K-calmodulin complex can be readded to ATP-treated, stripped microvillar cores. The resulting bundles display the same helical and periodic arrangement of lateral bridges as is found in vivo. In reconstitution experiments, actin filaments incubated in EGTA with purified fimbrin and villin form smooth-sided bundles containing an apparently random number of filaments. Upon addition of 110K-calmodulin complex, the bundles, as viewed by electron microscopy of negatively stained images, display along their entire length helically arranged projections with the same 33-nm repeat of the lateral cross-bridges found on microvilli in vivo; these bridges likewise tilt relative to the bundle. Thus, reconstitution of actin filaments with fimbrin, villin, and the 110K-calmodulin complex results in structures remarkably similar to native microvillar cores. These data provide direct proof that the 110K-calmodulin is the cross-bridge protein and indicate that actin filaments bundled by fimbrin and villin are of uniform polarity and lie in register. The arrangement of the cross-bridge arms on the bundle is determined by the structure of the core filaments as fixed by fimbrin and villin; a contribution from the membrane is not required.

Factors affecting movement of F-actin filaments propelled by skeletal muscle heavy meromyosin

1992 ◽  
Vol 262 (3) ◽  
pp. C714-C723 ◽  
Author(s):  
E. Homsher ◽  
F. Wang ◽  
J. R. Sellers
Keyword(s):  
Skeletal Muscle ◽  
Ionic Strength ◽  
Actin Filament ◽  
Molecular Motors ◽  
Actin Filaments ◽  
Heavy Meromyosin ◽  
Shortening Velocity ◽  
Weakly Bound ◽  
Factors Affecting ◽  
Cross Bridges

The measurement of fluorescent-labeled actin filament movement driven by mechanoenzymes (e.g., myosin) is an important methodology for the study of molecular motors. It is assumed that the filament velocity (Vf) is analogous to the unloaded shortening velocity (Vu) seen in muscle fibers. Methods are described to reproducibly quantitate the movement of these filaments and to select uniformly moving filaments and specify their Vf. Use of these techniques allowed comparison of Vf to literature values for Vu with regard to [ATP], [ADP], [Pi], pH, ionic strength (10-150 mM), and temperature (15-30 degrees C). Vf and Vu are quantitatively similar with respect to the effects of substrate and product concentrations and temperatures greater than 20 degrees C. However, Vf is more sensitive to decreases in pH and temperatures less than 20 degrees C than Vu. At ionic strengths of 50-150 mM, Vf and Vu exhibit similar ionic strength dependencies (decreasing with ionic strength). At ionic strengths less than 50 mM, Vf is markedly reduced. Results of experiments using adenosine 5'-O-(3-thiotriphosphate) suggest that increasing the number of weakly bound cross bridges does not seriously affect Vf. Thus, although Vf is a good analogue for Vu under certain conditions (elevated ionic strength and temperatures greater than 20 degrees C), under others it is not. The results of motility assays must be cautiously interpreted.

scholarly journals Structural organization of actin in the sea urchin egg cortex: microvillar elongation in the absence of actin filament bundle formation

1982 ◽  
Vol 93 (1) ◽  
pp. 24-32 ◽  
Author(s):  
DA Begg ◽  
LI Rebhun ◽  
H Hyatt
Keyword(s):  
Sea Urchin ◽  
Actin Filament ◽  
Actin Filaments ◽  
Calcium Ionophore ◽  
Ionophore A23187 ◽  
Acid Activation ◽  
Cytoplasmic Ph ◽  
Sea Urchin Egg ◽  
Filament Bundles ◽  
Filament Bundle

We have investigated the relationship between the formation of actin filament bundles and the elongation of microvilli (MV) after fertilization in sea urchin eggs. In a previous study (1979, J Cell Biol. 83:241-248) we demonstrated that increased pH induced the formation of actin filaments in isolated sea urchin egg cortices with the concomitant elongation of MV. On the basis of these results we suggested that increased cytoplasmic pH after fertilization causes a reorganization of cortical actin, which in turn provides the force for MV elongation. To test this hypothesis, we compared the morphology of microvilli in eggs activated with and without the release of fertilization acid. Activation of eggs in normal sea water with the calcium ionophore A23187 causes the release of fertilization acid and the elongation of MV containing core bundles of actin filaments. Eggs activated with A23187 in NA(+)-free water do not undergo normal fertilization acid release but develop elongated, flaccid MV. These MV contain an irregular network of actin filaments rather than the parallel bundles of filaments found in normal MV. The addition of 40 mM NaCl to these eggs results in the release of H(+) and the concomitant conversion of flaccid MV to erect MV containing typical core bundles of actin filaments. Identical results are obtained when 10 mM NH(4)Cl is substituted for NaCl. The induction of cytoplasmic alkalinization in unactivated eggs with NH(4)Cl does not cause either MV elongation or the formation of actin filament bundles . These results suggest that: (a) the elongation of MV is stimulated by a rise in intracellular free Ca(++) concentration; (b) actin filament bundle formation is triggered by an increase in cytoplasmic pH; and (c) the formation of actin filament bundles is not necessary for MV elongation but is required to provide rigid support for MV.

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.

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