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L G Tilney

Publications and source records attributed to L G Tilney.

At least 73 records · Page 4Linked to original sources

Actin filaments, stereocilia, and hair cells of the bird cochlea. IV. How the actin filaments become organized in developing stereocilia and in the cuticular plate.

In 8-day-old embryos stereocilia can be identified on the hair cells of the chick cochlea; within each is a small population of actin filaments which extend from the tip of the stereocilium to the apical cytoplasm of the cell. These filaments are not ordered in a regular way, however, and tend to be found near the lateral margins of the stereocilia with large spaces between adjacent filaments. By 9 days the spaces between adjacent filaments are reduced and there are regions where the crossover points of adjacent actin helices are in register even though in cross section the actin filaments do not lie on a regular lattice. By 10-11 days the actin filaments become progressively more crossbridged together and we can recognize in longitudinal section horizontal stripes caused by the periodicity of the crossbridges. In transverse section the filaments begin to lie on a hexagonal lattice. Each stereocilium, however, contains less than 100 actin filaments. Evidence is presented that once crossbridging is maximal and the filaments hexagonally packed (Days 11-12), the stereocilia increase in width by the orderly addition of actin filaments to the lateral margins of the existing filament bundle so that by Day 16 we find up to 400 filaments all packed on a hexagonal lattice. Thus there are two stages in bundle formation. In the first a small number of filaments condense into a hexagonally packed, crosslinked bundle. In the second, the bundle increases in diameter by addition of filaments to the periphery of the bundle in a process akin to crystal growth. From observations on the elongation of filaments in the rootlets and stereocilia, we conclude that rootlets grow by addition of subunits at the nonpreferred end while stereocilia elongate by addition to the preferred end. What makes this interesting is that these two modes of addition occur at different developmental times.

Actins↗

Functional organization of the cytoskeleton.

Within each stereocilium of chick hair cells is a hexagonally packed bundle of actin filaments. Diffraction patterns of thin sections of these bundles reveal that the actin filaments are aligned such that the crossover points of adjacent filaments are in transverse register. Since each actin filament is composed of subunits that are organized in a helical pattern, yet all the actin filaments are in transverse register, crossbridges between filaments can form only at positions dictated by the geometry of the actin helix or at 125 A intervals. Thus the crossbridges appear in electron micrographs as regularly spaced bands (125 A) that are perpendicular to the axis of the stereocilium. From examination of stereocilia of organisms who have a temporary threshold shift due to exposure to loud noise, we know that the integrity of the actin filaments and their crossbridges is essential for hair cell function. However, particularly interesting is that 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. Thus, resistance to bending or displacement must be a property of the number of bridges present which in turn is a function of the number and lengths of actin filaments present. 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. To try to understand how hair cells control the length and number of actin filaments per stereocilium and thus the length and width of the stereocilia, we examined cochlea in chick embryos of increasing maturity. Of interest is that very early in development (10-day embryos) the total hair cell number and position is specified. Thus it is possible to study the growth of stereocilia in cells whose final stereociliary length and width is already known. Stereocilia first elongate (from 8 to 11 days--first phase); they then stop elongating and increase in width (12-16 days--second phase), then elongate again (third phase) to the length appropriate to the position of the hair cell on the cochlea. During the first phase a few actin filaments are present, but initially poorly ordered.(ABSTRACT TRUNCATED AT 400 WORDS)

Actin Cytoskeleton↗

Acrosomal reaction of the Thyone sperm. III. The relationship between actin assembly and water influx during the extension of the acrosomal process.

In an attempt to investigate the role of water influx in the extension of the acrosomal process of Thyone sperm, we induced the acrosomal reaction in sea water whose osmolarity varied from 50 to 150% of that of sea water. (a) Video sequences of the elongation of the acrosomal processes were made; plots of the length of the acrosomal process as a function of (time)1/2 produced a straight line except at the beginning of elongation and at the end in both hypotonic and hypertonic sea water (up to 1.33 times the osmolarity of sea water), although the rate of elongation was fastest in hypotonic sea water and was progressively slower as the tonicity was raised. (b) Close examination of the video sequences revealed that regardless of the tonicity of the sea water, the morphology of the acrosomal processes were similar. (c) From thin sections of fixed sperm, the amount of actin polymerization that takes place is roughly coupled to the length of the acrosomal process formed so that sperm with short processes only polymerize a portion of the actin that must be present in those sperm. From these facts we conclude that the influx of water and the release of actin monomers from their storage form in the profilactin (so that these monomers can polymerize) are coupled. The exact role of water influx, why it occurs, and whether it could contribute to the extension of the acrosomal process by a hydrostatic pressure mechanism is discussed.

Acrosome↗

How to build a bend into an actin bundle.

The bundle of actin filaments in the sperm of the horseshoe crab has a polygonal form. This appearance results from regularly spaced, sharp bends (elbows) separated by straight segments (arms). We conclude that the elbows are built into the bundle by a rearrangement of interfilament crossbridges in the arms. The rearrangement, which makes used of the specific bonding properties of the crossbridges, is made possible by the helical symmetry of actin and by the hexagonal packing of the filaments. The angle of the bend (154 degrees) is fixed by the interfilament separation and the axial spacing of actin subunits within a filament. In the arms on either side of an elbow, rows of filaments slip relative to each other. The slippage, and hence the elbow, is locked in by an axial shift of the crossbridges between adjacent rows of filaments. The variable twist of actin filaments may be important in accommodating the strain of crossbridge rearrangement.

Actins↗

Phalloidin enhances actin assembly by preventing monomer dissociation.

Incubation of the isolated acrosomal bundles of Limulus sperm with skeletal muscle actin results in assembly of actin onto both ends of the bundles. These cross-linked bundles of actin filaments taper, thus allowing one to distinguish directly the preferred end for actin assembly from the nonpreferred end; the preferred end is thinner. Incubation with actin in the presence of equimolar phalloidin in 100 mM KCl, 1 mM MgCl2 and 0.5 mM ATP at pH 7.5 resulted in a slightly smaller association rate constant at the preferred end than in the absence of the drug (3.36 +/- 0.14 X 10(6) M-1 s-1 vs. 2.63 +/- 0.22 X 10(6) M-1 s-1, control vs. experimental). In the presence of phalloidin, the dissociation rate constant at the preferred end was reduced from 0.317 +/- 0.097 s-1 to essentially zero. Consequently, the critical concentration at the preferred end dropped from 0.10 microM to zero in the presence of the drug. There was no detectable change in the rate constant of association at the nonpreferred end in the presence of phalloidin (0.256 +/- 0.015 X 10(6) M-1 s-1 vs. 0.256 +/- 0.043 X 10(6) M-1 s-1, control vs. experimental); however, the dissociation rate constant was reduced from 0.269 +/- 0.043 s-1 to essentially zero. Thus, the critical concentration at the nonpreferred end changed from 1.02 microM to zero in the presence of phalloidin. Dilution-induced depolymerization at both the preferred and nonpreferred ends was prevented in the presence of phalloidin. Thus, phalloidin enhances actin assembly by lowering the critical concentration at both ends of actin filaments, a consequence of reducing the dissociation rate constants at each end.

Acrosome↗

Actin filaments, stereocilia, and hair cells of the bird cochlea. I. Length, number, width, and distribution of stereocilia of each hair cell are related to the position of the hair cell on the cochlea.

Located on the sensory epithelium of the sickle-shaped cochlea of a 7- to 10-d-old chick are approximately 5,000 hair cells. When the apical surface of these cell is examined by scanning microscopy, we find that the length, number, width, and distribution of the stereocilia on each hair cell are predetermined. Thus, a hair cell located at the distal end of the cochlea has 50 stereocilia, the longest of which are 5.5 microns in length and 0.12 microns in width, while those at the proximal end number 300 and are maximally 1.5 microns in length and 0.2 micron in width. In fact, if we travel along the cochlea from its distal to proximal end, we see that the stereocilia on successive hair cells gradually increase in number and width, yet decrease in length. Also, if we look transversely across the cochlea where adjacent hair cells have the same length and number of stereocilia (they are the same distance from the distal end of the cochlea), we find that the stereocilia of successive hair cells become thinner and that the apical surface area of the hair cell proper, not including the stereocilia, decreases from a maximum of 80 microns2 to 15 microns2. Thus, if we are told the length of the longest stereocilium on a hair cell and the width of that stereocilium, we can pinpoint the position of that hair cell on the cochlea in two axes. Likewise, if we are told the number of stereocilia and the apical surface of a hair cell, we can pinpoint the location of that cell in two axes. The distribution of the stereocilia on the apical surface of the cell is also precisely determined. More specifically, the stereocilia are hexagonally packed and this hexagonal lattice is precisely positioned relative to the kinocilium. Because of the precision with which individual hair cells regulate the length, width, number, and distribution of their cell extensions, we have a magnificent object with which to ask questions about how actin filaments that are present within the cell are regulated. Equally interesting is that the gradient in stereociliary length, number, width, and distribution may play an important role in frequency discrimination in the cochlea. This conclusion is amplified by the information presented in the accompanying paper (Tilney, L.G., E.H. Egelman, D.J. DeRosier, and J.C. Saunders, 1983, J. Cell Biol., 96:822-834) on the packing of actin filaments in this stereocilia.

Animals↗

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.

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.

Animals↗

Actin from Thyone sperm assembles on only one end of an actin filament: a behavior regulated by profilin.

Thyone sperm were demembranated with Triton X-100 and, after washing, extracted with 30 mM Tris at pH 8.0 and 1 mM MgCl2. After the insoluble contaminants were removed by centrifugation, the sperm extract was warmed to 22 degrees C. Actin filaments rapidly assembled and aggregated into bundles when KCl was added to the extract. When we added preformed actin filaments, i.e., the acrosomal filament bundles of Limulus sperm, to the extract, the actin monomers rapidly assembled on these filaments. What was unexpected was that assembly took place on only one end of the bundle--the end corresponding to the preferred end for monomer addition. We showed that the absence of growth on the nonpreferred end was not due to the presence of a capper because exogenously added actin readily assembled on both ends. We also analyzed the sperm extract by SDS gel electrophoresis. Two major proteins were present in a 1:1 molar ratio: actin and a 12,500-dalton protein whose apparent isoelectric point was 8.4. The 12,500-dalton protein was purified by DEAE chromatography. We concluded that it is profilin because of its size, isoelectric point, molar ratio to actin, inability to bind to DEAE, and its effect on actin assembly. When profilin was added to actin in the presence of Limulus bundles, addition of monomers on the nonpreferred end of the bundle was inhibited, even though actin by itself assembled on both ends. Using the Limulus bundles as nuclei, we determined the critical concentration for assembly off each end of the filament and estimated the Kd for the profilin-actin complex (approximately 10 microM). We present a model to explain how profilin may regulate the extension of the Thyone acrosomal process in vivo: The profilin-actin complex can add to only the preferred end of the filament bundle. Once the actin monomer is bound to the filament, the profilin is released, and is available to bind to additional actin monomers. This mechanism accounts for the rapid rate of filament elongation in the acrosomal process in vivo.

Actins↗

Under physiological conditions actin disassembles slowly from the nonpreferred end of an actin filament.

Incubation of the isolated acrosomal bundles of Limulus sperm with skeletal muscle actin results in assembly of actin onto both ends of the bundles. Because of the taper of these cross-linked bundles of actin filaments, one can distinguish directly the preferred end for assembly from the nonpreferred end. Loss of growth with time from the nonpreferred end was directly assessed by electron microscopy and found to be dependent upon salt concentration. Under physiological conditions (100 mM KCl, 1 mM MgCl2) and excess ATP (0.5 mM), depolymerization of the newly assembled actin filaments at the nonpreferred end over an 8-h period was 0.024 micron/h. Thus, even after 8 h, 63% of the bundles retained significant growth on their nonpreferred ends, the average length being 0.21 micron +/- 0.04. However, in the presence of 1.2 mM CaCl2, disassembly of actin monomers from the nonpreferred end increased substantially. By 8 h, only 7% of the bundles retained any actin growth on the nonpreferred ends, and the depolymerization rate off the nonpreferred end was 0.087 micron/h. From these results we conclude that, in the absence of other cellular factors, disassembly of actin subunits from actin filaments (subunit exchange) is too slow to influence most of the motile events that occur in cells. We discuss how this relates to treadmilling.

Acrosome↗

Changes in the organization of actin filaments in the stereocilia of noise-damaged lizard cochleae.

Alligator lizards exposed to 105 dB broadband noise for 24 h showed a 33 dB loss in hearing which was almost completely recovered 11 days after removal from the noise. Two lesions were found in the actin filament organization which could affect the rigidity of the stereocilia and thus could account for this hearing loss. These lesions preferentially affect the tallest stereocilia. The more common one is a depolymerization of the actin filaments at the base of the stereocilium where it makes contact with the cuticular plate. This results in a displacement and detachment of the stereocilium from its rootlet, thereby affecting the orientation of the tallest stereocilium. The other lesion involves a loss in crossbridges between adjacent actin filaments in the stereocilium. We demonstrate that such a loss will dramatically affect the rigidity of the stereocilia.

Actins↗

A change in twist of actin provides the force for the extension of the acrosomal process in Limulus sperm: the false-discharge reaction.

One of the most spectacular motions is the generation of the acrosomal process in the limulus sperm. On contact with the egg, the sperm generates a 60-mum-long process that literally drills its way through the jelly surrounding the egg. This irresversible reaction takes only a few seconds. We suggested earlier that this motion is driven by a change in twist of the actin filaments comprising the acrosomal process. In this paper we analyze the so-called false discharge, a reversible reaction, in which the acrosomal filament bundle extends laterally from the base of the sperm and not anteriorly from the apex. Unlike the true discharge, which is straight, the false discharge is helical. Before extension, the filament bundle is coiled about the base of the sperm. In the coil, the bundle is not smoothly bent but consists of arms (straight segments) and elbows (corners) so that the coil looks like a 14-sided polygon. The extension of the false discharge works as follows: starting at the base of the bundle, the filaments change their twist which concomitantly changes the orientations of the elbows relative to each other; that is, in the coil, the elbows all like in a common plane, but after the change in twist, the plane of each elbow is rotated to be perpendicular to that of its neighbors. This change transforms the bundle from a compact coil into an extended left- handed helix. Because the basal end of the bundle is unconstrained, the extension is lateral. The true discharge works the same way but starts at the apical end of the bundle. The apical end, however, is constrained by its passage through the nuclear canal, which directs the extention anteriorly. Unlike the false discharge, during the true discharge the elbows are melted out, making the reaction irreversible. This study shows that rapid movement can be regenerated by actin without myosin and gives us insight into the molecular mechanism.

Actins↗

Acrosomal reaction of thyone sperm. I. Changes in the sperm head visualized by high resolution video microscopy.

Structural changes inside the head of Thyone sperm undergoing the acrosomal reaction were followed with a high-resolution, differential interference contrast (DIC) video microscope. The beating sperm, adhering by their midpiece to the cover slip of a wedge perfusion chamber, were activated by a calcium ionophore (20 microM A23187) suspended in sea water containing 50 mM excess CaCl2. Before activation of the sperm, the acrosomal region appears as a 1.1-microM diameter sphere, slightly less dense than the rest of the sperm head. Upon activation, the acrosome pops; the acrosomal region suddenly swells and its refractive index drops. After approximately 1 s, a crescent-shaped periacrosomal cup appears behind the acrosomal vacuole. In the next several seconds, the cup loses more refractive index and expands forward as the acrosomal process extends. The acrosomal vacuole becomes smaller, but without appreciable drop in refractive index. These observations, coupled with the behavior of the extending acrosomal process reported in the companion paper, and in electron microscopy (EM) and early physiological studies, suggest that the acrosomal process is extended by a combination of the explosive polymerization of actin and the osmotic swelling of the periacrosomal cup material. In this paper, we also consider the meaning of the enhanced DIC image seen in the high-resolution video microscope, and discuss the reliability of measurements on small linear dimensions made with the DIC microscope.

Acrosome↗

Acrosomal reaction of Thyone sperm. II. The kinetics and possible mechanism of acrosomal process elongation.

Thyone sperm were induced to undergo the acrosomal reaction with a calcium ionophore A23187 in sea water containing 50 mM excess CaCl2, and the extension of the acrosomal process was recorded with high-resolution, differential interference contrast video microscopy at 60 fields/sec. The length of the acrosomal process was measured at 0.25-s intervals on nine sperm. When the data were plotted as (length)2 vs. time, the points fell exactly on a straight line except for the initial and very final stages of elongation. Cytochalasin B alters the rate of elongation of the acrosomal process in a dose-dependent way, inhibiting the elongation completely at high concentrations (20 micrograms/ml). However, no inhibition was observed unless excess Ca++ was added to sea water. The concentration of actin in the periacrosomal cup of the unreacted sperm is as high as 160 mg/ml; we calculate this concentration from the number and lengths of the actin filaments in a fully reacted sperm, and the volume of the periacrosomal cup in the unreacted sperm. These results are consistent with the hypothesis proposed earlier that monomers add to the ends of the actin filaments situated at the tip of the growing acrosomal process (the preferred end for monomer addition), and that the rate of elongation of the process is limited by diffusion of monomers from the sperm head (periacrosomal cup) to the tip of the elongating process. During the extension of the acrosomal process, a few blebs distributed along its lengths move out with the process. These blebs maintain a constant distance from the tip of the growing process. At maximum length, the straight acrosomal process slackens into a bow, and numerous new blebs appear. A few seconds later, the process suddenly straightens out again and sometimes actually contracts. The behavior of the blebs indicates that membrane is inserted at the base of the growing acrosomal process, and that membrane assembly and water uptake must be coupled to actin assembly during elongation. We discuss how the dynamic balance of forces seems to determine the shape of the growing acrosomal process, and how actin assembly may be controlled during the acrosomal reaction.

Acrosome↗

Organization of actin, myosin, and intermediate filaments in the brush border of intestinal epithelial cells.

Terminal webs prepared from mouse intestinal epithelial cells were examined by the quick-freeze, deep-etch, and rotary-replication method. The microvilli of these cells contain actin filaments that extend into the terminal web in compact bundles. Within the terminal web these bundles remain compact; few filaments are separated from the bundles and fewer still bend towards the lateral margins of the cell. Decoration with subfragment 1 (S1) of myosin confirmed that relatively few actin filaments travel horizontally in the web. Instead, between actin bundles there are complicated networks of the fibrils. Here we present two lines of evidence which suggest that myosin is one of the major cross-linkers in the terminal web. First, when brush borders are exposed to 1 mM ATP in 0.3 M KCl, they lose their normal ability to bind antimyosin antibodies as judged by immunofluorescence, and they lose the thin fibrils normally found in deep-etch replicas. Correspondingly, myosin is released into the supernatant as judged by SDS gel electrophoresis. Second, electron microscope immunocytochemistry with antimyosin antibodies followed by ferritin-conjugated second antibodies leads to ferritin deposition mainly on the fibrils at the basal part of rootlets. Deep-etching also reveals that the actin filament bundles are connected to intermediate filaments by another population of cross-linkers that are not extracted by ATP in 0.3 M KCl. From these results we conclude that myosin in the intestinal cell may not only be involved in a short range sliding-filament type of motility, but may also play a purely structural role as a long range cross-linker between microvillar rootlets.

Actins↗

Interactions between actin filaments and between actin filaments and membranes in quick-frozen and deeply etched hair cells of the chick ear.

Replicas of the apical surface of hair cells of the inner ear (vestibular organ) were examined after quick freezing and rotary shadowing. With this technique we illustrate two previously undescribed ways in which the actin filaments in the stereocilia and in the cuticular plate are attached to the plasma membrane. First, in each stereocilium there are threadlike connectors running from the actin filament bundle to the limiting membrane. Second, many of the actin filaments in the cuticular plate are connected to the apical cell membrane by tiny branched connecting units like a "crow's foot." Where these "feet" contact the membrane there is a small swelling. These branched "feet" extend mainly from the ends of the actin filaments but some connect the lateral surfaces of the actin filaments as well. Actin filaments in the cuticular plate are also connected to each other by finer filaments, 3 nm in thickness and 74 +/- 14 nm in length. Interestingly, these 3-nm filaments (which measure 4 nm in replicas) connect actin filaments not only of the same polarity but of opposite polarities as documented by examining replicas of the cuticular plate which had been decorated with subfragment 1 (S1) of myosin. At the apicolateral margins of the cell we find two populations of actin filaments, one just beneath the tight junction as a network, the other at the level of the zonula adherens as a ring. The latter which is quite substantial is composed of actin filaments that run parallel to each other; adjacent filaments often show opposite polarities, as evidenced by S1 decoration. The filaments making up this ring are connected together by the 3-nm connectors. Because of the polarity of the filaments this ring may be a "contractile" ring; the implications of this is discussed.

Actins↗