Evaluation of various methods of measurement of the microtubule length in the cytoplasm of cultured cells

It is generally assumed that microtubules in tissue culture cells extend from the centrosome to cell periphery, and the length of individual microtubules averages several dozens of microns. However, direct electron-microscopic measurements have cast some doubt on this assumption. In this study, the average length of microtubules in cultured Vero cells was estimated using a combined approach. The length of free cytoplasmic and centrosomal microtubules was determined by means of electron microscopy in serial sections; concurrently, the length of free microtubules in the lamella was measured in preparations stained with tubulin antibodies (an indirect immunofluorescent method), by tracing saltatory particle movements along the microtubules in living cells. According to the data of immunofluorescent microscopy, microtubule length in the lamella averaged 4.57 +/- 3.69 microns. However, since two or more microtubules can overlap, their length may be slightly overestimated by this method. On the other hand, saltatory movements are easy to monitor and measure fairly accurately, but their range may be shorter than the actual microtubule length because of a limited processiveness of motors (kinesin and dynein). On average, the trajectories of saltatory movements in living cells were 3.85 +/- 0.72 microns long. At the electron-microscopic level, microtubule length was analyzed using pseudo-three-dimensional reconstructions of the microtubule systems around the centrosome and in the lamella. The length of free microtubules in the lamella reached 18 microns, averaging 3.33 +/- 2.43 microns; the average length of centrosomal microtubules was 1.49 +/- 0.82 microns. Good correspondence between the data on microtubule length and arrangement obtained by different methods allows the conclusion that most of free microtubules in Vero cells actually have a length of 2-5 microns; i.e., they are much shorter than the cell radius (about 25 microns). Microtubules extending from the centrosome are shorter still and do not reach the cell periphery. Thus, most microtubules in the lamella of Vero cells are free and their ordered arrangement is not associated with their attachment to the centrosome.     

Involvement of microtubules in the regulation of neuronal growth cone morphologic remodeling

The guidance of nerve fibers depends on the constant protrusion, movement, and retraction (i.e., remodeling) of growth cone lamellae and filopodia. We used drugs that interfere with the dynamics of microtubules to investigate the role of microtubules in the remodeling of larval amphibian spinal cord neuronal growth cones. Vinblastine (8–100 nM), taxol (10 nM), and nocodazole (330 nM) altered microtubule distributions in growth cones and decreased the percentage of lamellar perimeter undergoing remodeling, while not affecting the rates of lamellar protrusion and retraction. Also, 8–20 nM vinblastine caused temporary losses of the continuity of the originally fan-shaped lamella, resulting in two or more lamellae at the growth cone. At higher concentrations of microtubule drugs, the originally fan-shaped lamella broke up into separate smaller lamellae followed by the centrifugal displacement from the base of the growth cone and eventual collapse of the resultant lamellae. Low doses of cytochalasin B prevented the centrifugal displacement of lamellae in response to microtubule drugs. During microtubule drug-mediated loss of growth cone lamellae, some filopodia were observed to elongate to greater than normal lengths. Similarly, exposure to 20 nM vinblastine resulted in an increase in filopodial length but not filopodial number. As evidenced by DiOC₆(3) staining, 8–20 nM vinblastine altered the distribution of membranous organelles within growth cones, suggesting that the effects of microtubule drugs on growth cones may be mediated in part by alterations in organelle localization. Our data show that microtubules are involved in the maintenance and regulation of lamellar and filopodial structures at the neuronal growth cone. These findings have implications for the mechanisms by which growth cones are guided during development and regeneration. © 1998 John Wiley & Sons, Inc. J Neurobiol 35: 121–140, 1998     

The organization of F-actin and microtubules in growth cones exposed to a brain-derived collapsing factor

In previous work we characterized a brain derived collapsing factor that induces the collapse of dorsal root ganglion growth cones in culture (Raper and Kapfhammer, 1990). To determine how the growth cone cytoskeleton is rearranged during collapse, we have compared the distributions of F-actin and microtubules in normal and partially collapsed growth cones. The relative concentration of F-actin as compared to all proteins can be measured in growth cones by rationing the intensity of rhodamine-phalloidin staining of F-actin to the intensity of a general protein stain. The relative concentration of F- actin is decreased by about one half in growth cones exposed to collapsing factor for five minutes, a time at which they are just beginning to collapse. During this period the relative concentration of F-actin in the leading edges of growth cones decreases dramatically while the concentration of F-actin in the centers decreases little. These results suggest that collapse is associated with a net loss of F- actin at the leading edge. The distributions of microtubules in normal and collapsing factor treated growth cones were examined with antibodies to tyrosinated and detyrosinated isoforms of alpha-tubulin. The tyrosinated form is found in newly polymerized microtubules while the detyrosinated form is not. The relative proximal-distal distributions of these isoforms are not altered during collapse, suggesting that rates of microtubule polymerization and depolymerization are not greatly affected by the presence of collapsing factor. An analysis of the distributions of microtubules before and after collapse suggests that microtubules are rearranged, but their polymerization state is unaffected during collapse. These results are consistent with the hypothesis that the brain derived collapsing factor has little effect on microtubule polymerization or depolymerization. Instead it appears to induce a net loss of F-actin at the leading edge of the growth cone.     

The dynamics of microtubule repolymerization in a cell: rapid growth from the centrosome and slow recovery of free microtubules

According to the current view, the microtubule system in animal cells consists of two components: microtubules attached to the centrosome (these microtubules stretch radially towards the cell margin), and free microtubules randomly distributed in the cytoplasm without visible association with any microtubule-organizing centers. The ratio of the two sets of microtubules in the whole microtubule array is under discussion. Addressing this question, we have analysed the recovery of microtubules in cultured Vero nucleated cells and cytoplasts, with and without centrosomes in these. Cells were fixed at different time points, and individual microtubules were traced on serial optical sections. During a slow recovery after cold treatment (4 degrees C, for 4 h; recovery at 30 degrees C) polymerization of microtubules started mainly from the centrosome. At early stages of recovery the share of free microtubules made about 10% of all microtubules, and their total length increased slower than the lenght of centrosome-attached microtubules. During a rapid recovery after nocodazole treatment (10 microg/ml, 2 h; recovery in drug-free medium at 37 degrees C), the share of free microtubules was about 35%, but their total length increased slower than the length of centrosome-attached microtubules. In 6-8 min (rapid recovery) or 12-16 min (slow recovery), tips of centrosomal microtubules reached the cell margin, and their increased density made it impossible to recognize individual microtubules. However, under the same conditions in cytoplasts without centrosomes the normal number of microtubules recovered only in 60 min, which enabled us to suppose that the complete recovery of microtubule system in the whole cells may be also rather long. When the first centrosomal microtubules reached the cell margin, the optical density of microtubules started to decrease from the centrosome region towards the cell margin, according to the exponential curve. Later on, the optical density in the centrosome region and near the cell margin remained at the same level, but microtubule density increased in the middle part of the cell, and in 45-60 min the plot of the optical density vs the distance from the centrosome became linear, as in control cells. Since no significant curling of microtubules occurs near the cell margin, the density of microtubules in the endoplasm may increase due only to polymerization of free microtubules. We suppose that in cultured cells the microtubule network recovery proceeds in two stages. At the initial stage, a rapid growth of centrosomal microtubules takes place in addition to the turnover of free microtubules with unstable minus ends. At the second stage, when microtubule growth from the centrosome becomes limited by the cell margin, a gradual extension of free microtubules occurs in the internal cytoplasm.     

Observation and quantification of individual microtubule behavior in vivo: microtubule dynamics are cell-type specific

Recent experiments have demonstrated that the behavior of the interphase microtubule array is cell-type specific: microtubules in epithelial cells are less dynamic than microtubules in fibroblasts (Pepper-kok et al., 1990; Wadsworth and McGrail, 1990). To determine which parameters of microtubule dynamic instability behavior are responsible for this difference, we have examined the behavior of individual microtubules in both cell types after injection with rhodamine-labeled tubulin subunits. Individual microtubules in both cell types were observed to grow, shorten, and pause, as expected. The average amount of time microtubules remained within the lamellae of CHO fibroblasts, measured from images acquired at 10-s intervals, was significantly shorter than the average amount of time microtubules remained within lamellae of PtK1 epithelial cells. Further analysis of individual microtubule behavior from images acquired at 2-s intervals reveals that microtubules in PtK1 cells undergo multiple brief episodes of growth and shortening, resulting in little overall change in the microtubule network. In contrast, microtubules in lamellae of CHO fibroblasts are observed to undergo fewer transitions which are of longer average duration, resulting in substantial changes in the microtubule network over time. A small subset of more stable microtubules was also detected in CHO fibroblasts. Quantification of the various parameters of dynamic instability behavior from these sequences demonstrates that the average rates of both growth and shortening are significantly greater for the majority of microtubules in fibroblasts than for microtubules in epithelial cells (19.8 +/- 10.8 microns/min, 32.2 +/- 17.7 microns/min, 11.9 +/- 6.5 microns/min, and 19.7 +/- 8.1 microns/min, respectively). The frequency of catastrophe events (1/interval between catastrophe events) was similar in both cell types, but the frequency of rescue events (1/time spent shrinking) was significantly higher in PtK1 cells. Thus, individual microtubules in PtK1 lamellae undergo frequent excursions of short duration and extent, whereas most microtubules in CHO lamellae undergo more extensive excursions often resulting in the appearance or disappearance of microtubules within the field of view. These observations provide the first direct demonstration of cell-type specific behavior of individual microtubules in living cells, and indicate that these differences can be brought about by modulation of the frequency of rescue. These results directly support the view that microtubule dynamic instability behavior is regulated in a cell-type specific manner.     

Quantitative analysis of microtubule dynamics during adhesion-mediated growth cone guidance

During adhesion-mediated neuronal growth cone guidance microtubules undergo major rearrangements. However, it is unknown whether microtubules extend to adhesion sites because of changes in plus-end polymerization and/or translocation dynamics, because of changes in actin-microtubule interactions, or because they follow the reorganization of the actin cytoskeleton. Here, we used fluorescent speckle microscopy to directly quantify microtubule and actin dynamics in Aplysia growth cones as they turn towards beads coated with the cell adhesion molecule apCAM. During the initial phase of adhesion formation, dynamic microtubules in the peripheral domain preferentially explore apCAM-beads prior to changes in growth cone morphology and retrograde actin flow. Interestingly, these early microtubules have unchanged polymerization rates but spend less time in retrograde translocation due to uncoupling from actin flow. Furthermore, microtubules exploring the adhesion site spend less time in depolymerization. During the later phase of traction force generation, the central domain advances and more microtubules in the peripheral domain extend because of attenuation of actin flow and clearance of F-actin structures. Microtubules in the transition zone and central domain, however, translocate towards the adhesion site in concert with actin arcs and bundles, respectively. We conclude that adhesion molecules guide neuronal growth cones and underlying microtubule rearrangements largely by differentially regulating microtubule-actin coupling and actin movements according to growth cone region and not by controlling plus-end polymerization rates.     

Spatial organization of centrosome-attached and free microtubules in 3T3 fibroblasts

The spatial organization of microtubules is crucial for different cellular processes. It is traditionally supposed that fibroblasts have radial microtubule arrays consisting of long microtubules that run from the centrosome. However, a detailed analysis of the microtubule array in the internal cytoplasm has never been performed. In the current study, we used laser photobleaching to analyze the spatial organization of microtubules in the internal cytoplasm of cultured 3T3 fibroblasts. Cells were injected with Cy-3-labeled tubulin, after which the growth of microtubules in the centrosome region and peripheral parts of cytoplasm was assayed in the bleached zone. In most cases, microtubule growth in the bleached zone occurred rectilinearly; at distances of up to 5 μm, microtubules seldom bend more than 10°–15°. We considered a growing fragment of the microtubule as a vector with the beginning at the point of occurrence and the end at the point where the growth terminated (or the end point after 30 s if microtubule persistent growth proceeded for longer). We defined the direction of microtubule growth in different parts of the cell using these vectors and measured the angle of their deviation from the vector of comparison. In the area of the centrosome, we directed a comparison vector inside the bleached zone from the centrosome to the beginning of the growing microtubule segment; in the lamella and trailing part of the fibroblast, we used the vector of comparison directed along the long axis of the cell from its geometrical center to periphery. The microtubules growing straight away from the centrosome grew along the cell radius. However, at a distance of 10 μm from the centrosome, radially growing microtubules comprised 40% of the overall number, while at a distance of 20 μm, they made up only 25%. The rest of the microtubules grew in different directions, with the preferred angle between their growth direction and cell radius equaling around 90 °. In the lamella and trailing part of the fibroblast, 80% of all microtubules grew along the long axis of the cell or at an angle of no more than 20 °; 10–15% of microtubules grew along axis of the cell but towards the centrosome. Thus, in 3T3 fibroblasts, the radial system of microtubules is perturbed starting at a distance of several microns from the centrosome. In the internal cytoplasm, the microtubule system is completely disordered and, in the stretched parts of the polarized cell (lamella, trailing edge), the microtubule system again becomes well organized; microtubules are preferentially oriented along the long axis of the cell. From the results obtained, we conclude that the orderliness of microtubules at the periphery of the fibroblast is not a consequence of their growth from the centrosome; rather, their orientation is preset by local factors.     

Microtubule dynamics in cultured cells

The behavior of microtubules in cultured cells in a cooled matrix after the microinjection of fluorescent tubulin was studied using a frame recording by a digital camcorder. In the cell lamella, thepositive ends of individual microtubules extend and shorten at random. The histograms of rate distribution have an almost normal distribution with a mode around 0. The maximum rate of lengthening and shortening reaches 30 and 50 microns/min, respectively. The positive ends of microtubules in PtK1 cells were in an equilibrium state, while in murine embryonic fibroblasts and Vero cells, they were displaced, usually, to the cell edge. Free microtubules were present in the cells of all three cultures. In the epithelial cells, they were numerous and relatively stable, while in the fibroblasts, they occurred rarely and were depolymerized at the proximal end. Free microtubules in PtK1 cells appeared, mostly due to spontaneous assembly in the cytoplasm, not in the relationship with the preexisting microtubules, and, more rarely, due to breakage of long microtubules. Separation of microtubules from the centrosome is a very rare event. Unlike positive ends that were characterized by dynamic instability, negative ends were stable and were sometimes depolymerized. When long microtubules were broken, new negative ends were formed that were, as a rule, stable, while in the lamella of fibroblasts (in murine embryonic fibroblasts and Vero cells), new negative ends were immediately depolymerized: free microtubules existed in these cells no more than 1-2 min. A diffusion model has been proposed where the behavior of microtubule ends is considered as unidimensional diffusion. The coefficient of diffusion of positive ends in the epithelial cells is several times less than in the fibroblasts, thus suggesting a higher rate of tubulin metabolism in the fibroblasts, as compared to the epithelium. The results obtained indicate that for the exchange of long microtubules, the dynamic instability is not sufficient. In the fibroblasts, their exchange takes place, mostly, at the expense of depolymerization of the liberating negative ends, which agrees with the previously proposed conveyer hypothesis of microtubule assembly on the centrosome.     

Assembly and disassembly of axonal microtubules of the toad Xenopus laevis under the effect of temperature.

In toads Xenopus laevis living at 11 degrees (winter), the microtubular density of 4-microns myelinated axons of lumbosacral nerves was assessed with the electron microscope. In controls, the density was 11.2 microtubules/microns2. In nerves incubated at 0 degrees, microtubules decreased following a simple exponential curve with a half time of 4.7 min (k = 0.149 min-1); residual microtubules were 4.5%. After rewarming, the full complement of microtubules reappeared within 60 min. In steady state, the microtubular density exhibited a linear relationship with temperature (range: 0-22 degrees; slope 0.94 microtubules/microns 2 per degree; r, 0.96). After heating the nerve by 11 degrees above the physiological temperature, microtubules increased by 83%, whereby the pool of unpolymerized tubulin was at least 2.7 mg/ml of axoplasm. A seasonal variation of the microtubular density was observed which accorded with the environmental temperature. The macroscopic kinetics of microtubule disassembly in the axoplasm is similar to that reported for purified tubulin but that of assembly is slower. Microtubules of peripheral axons of Xenopus are cold-labile and vary during the annual cycle.     

Differences in the organization of actin in the growth cones compared with the neurites of cultured neurons from chick embryos

Sensory neurons from chick embryos were cultured on substrata that support neurite growth, and were fixed and prepared for both cytochemical localization of actin and electron microscopic observation of actin filaments in whole-mounted specimens. Samples of cells were treated with the detergent Triton X-100 before, during, or after fixation with glutaraldehyde to determine the organization of actin in simpler preparations of extracted cytoskeletons. Antibodies to actin and a fluorescent derivative of phallacidin bound strongly to the leading margins of growth cones, but in neurites the binding of these markers for actin was very weak. This was true in all cases of Triton X- 100 treatment, even when cells were extracted for 4 min before fixation. In whole-mounted cytoskeletons there were bundles and networks of 6-7-nm filaments in leading edges of growth cones but very few 6-7-n filaments were present among the microtubules and neurofilaments in the cytoskeletons of neurites. These filaments, which are prominent in growth cones, were identified as actin because they were stabilized against detergent extraction by the presence of phallacidin or the heavy meromyosin and S1 fragments of myosin. In addition, heavy meromyosin and S1 decorated these filaments as expected for binding to F-actin. Microtubules extended into growth cone margins and terminated within the network of actin filaments and bundles. Interactions between microtubule ends and these actin filaments may account for the frequently observed alignment of microtubules with filopodia at the growth cone margins.     

High voltage electron stereomicroscopy of the cilium-stereociliary complex of perioral sensory cells in Hydra

The cilium-stereociliary complex in perioral neurons of Hydra was examined by electron microscopy, with emphasis on stereomicrographs of serial, 0.5 micron thick, longitudinal and transverse sections. Longitudinal sections revealed (1) flat-topped cones in which the cilium was bent and the ciliary chamber appeared heart-shaped, and (2) pointed cones in which the cilium was straight and the ciliary chamber appeared triangular. Transverse sections revealed 10-12 stereocilia forming a cone over a central cilium with nine peripheral doublets of microtubules but with often more than two central microtubules. The ciliary membrane was fluted; fine filaments connected the outfoldings of membrane with the center of the microtubule doublets. Thin sections revealed 7 nm microfilaments in the stereocilia cores which branched basally into thick and thin roots; the thick roots surrounded the base of the central cilium. The cilium-stereociliary complex was enveloped by an epitheliomuscular cell sheath with a free margin distally and a septate junction proximally. In flat-topped cones the free margin of the enveloping epitheliomuscular cell was closely applied to the top of the cilium-stereociliary complex, whereas in pointed cones the cilium-stereociliary complex projected above the free margin of the sheath. Thus, the 7 nm actin-like filaments in the stereocilia might function to contract and open the complex in response to favorable stimuli so that the cilium is in contact with the aqueous environment.     

Estimation of the diffusion-limited rate of microtubule assembly.

Microtubule assembly is a complex process with individual microtubules alternating stochastically between extended periods of assembly and disassembly, a phenomenon known as dynamic instability. Since the discovery of dynamic instability, molecular models of assembly have generally assumed that tubulin incorporation into the microtubule lattice is primarily reaction-limited. Recently this assumption has been challenged and the importance of diffusion in microtubule assembly dynamics asserted on the basis of scaling arguments, with tubulin gradients predicted to extend over length scales exceeding a cell diameter, approximately 50 microns. To assess whether individual microtubules in vivo assemble at diffusion-limited rates and to predict the theoretical upper limit on the assembly rate, a steady-state mean-field model for the concentration of tubulin about a growing microtubule tip was developed. Using published parameter values for microtubule assembly in vivo (growth rate = 7 microns/min, diffusivity = 6 x 10(-12) m2/s, tubulin concentration = 10 microM), the model predicted that the tubulin concentration at the microtubule tip was approximately 89% of the concentration far from the tip, indicating that microtubule self-assembly is not diffusion-limited. Furthermore, the gradients extended less than approximately 50 nm (the equivalent of about two microtubule diameters) from the microtubule tip, a distance much less than a cell diameter. In addition, a general relation was developed to predict the diffusion-limited assembly rate from the diffusivity and bulk tubulin concentration. Using this relation, it was estimated that the maximum theoretical assembly rate is approximately 65 microns/min, above which tubulin can no longer diffuse rapidly enough to support faster growth.     

Microtubule dynamics differentially regulates Rho and Rac activity and triggers Rho-independent stress fiber formation in macrophage polykaryons

Multinucleated giant cells (MNGC) derived from avian peripheral blood monocytes present a dense microtubular network emanating from peripherally located centrosomes. We were interested to study how microtubule and F-actin cytoskeletons cooperate in MNGC to maintain cell shape. Microtubule depolymerization by nocodazole triggered the reorganization of the F-actin cytoskeleton in MNGC that is normally organized into podosomes, cortical actin filaments and membrane ruffles. After nocodazole treatment, F-actin was redistributed into unusual transverse fibers associated with focal adhesion plaques. When microtubules were allowed to repolymerize after nocodazole removal, F-actin appeared transiently, together with the small GTPase Rac, in large membrane ruffles. Using affinity precipitation assays, we show that microtubule depolymerization leads to activation of Rho and inhibition of Rac, whereas microtubule repolymerization induces Rac activation and Rho inhibition. Thus, the level of microtubule polymerization inversely regulates Rho and Rac activity in MNGC. Moreover, using C3 exoenzyme, a known inhibitor of Rho, we demonstrate that both the F-actin fiber formation in response to microtubule depolymerization and the formation of membrane ruffles after microtubule repolymerization occur in C3-treated MNGC, indicating that Rho is not required for these events.     

Protein kinase C activation promotes microtubule advance in neuronal growth cones by increasing average microtubule growth lifetimes

We describe a novel mechanism for protein kinase C regulation of axonal microtubule invasion of growth cones. Activation of PKC by phorbol esters resulted in a rapid, robust advance of distal microtubules (MTs) into the F-actin rich peripheral domain of growth cones, where they are normally excluded. In contrast, inhibition of PKC activity by bisindolylmaleimide and related compounds had no perceptible effect on growth cone motility, but completely blocked phorbol ester effects. Significantly, MT advance occurred despite continued retrograde F-actin flow-a process that normally inhibits MT advance. Polymer assembly was necessary for PKC-mediated MT advance since it was highly sensitive to a range of antagonists at concentrations that specifically interfere with microtubule dynamics. Biochemical evidence is presented that PKC activation promotes formation of a highly dynamic MT pool. Direct assessment of microtubule dynamics and translocation using the fluorescent speckle microscopy microtubule marking technique indicates PKC activation results in a nearly twofold increase in the typical lifetime of a MT growth episode, accompanied by a 1.7-fold increase and twofold decrease in rescue and catastrophe frequencies, respectively. No significant effects on instantaneous microtubule growth, shortening, or sliding rates (in either anterograde or retrograde directions) were observed. MTs also spent a greater percentage of time undergoing retrograde transport after PKC activation, despite overall MT advance. These results suggest that regulation of MT assembly by PKC may be an important factor in determining neurite outgrowth and regrowth rates and may play a role in other cellular processes dependent on directed MT advance.     

Role of cytoskeleton in cell shaping of developing mesophyll of wheat (Triticum aestivum L.).

The effects of oryzalin and cytochalasin B (CB) on microtubule and actin microfilament arrays and on cell shaping were investigated in developing wheat mesophyll. Excised immature leaf sections capable of differentiating were incubated with the drugs. The behavior of the cytoskeleton was monitored by fluorescence microscopy after labeling with fluorescent dyes. Brief incubation with oryzalin (40 min, 10 microM) caused disassembly of microtubules. Recovery of microtubule arrays was comparatively slow after removal of the drug. Cells failed to establish transverse cortical bands of microtubules and transverse hoops of wall reinforcement. They expanded isodiametrically rather than longitudinally without forming lobes typical of wheat mesophyll cells. Brief treatment with CB (60 min, 20 micrograms ml-1) appeared to disrupt the microfilament arrays. Filaments recovered rapidly after removal of CB, and cells were able to shape in an apparently normal fashion. Continuous incubation at comparatively low concentration of CB (4 micrograms ml-1) appeared to cause selective loss of the fine transverse cortical microfilament arrays. Cortical transverse microtubule arrays persisted, but failed to form distinct bands in the majority of the cells. Cells were able to elongate in an almost normal fashion, but no lobes were formed.     

Microtubules remodel actomyosin networks in Xenopus egg extracts via two mechanisms of F-actin transport

Interactions between microtubules and filamentous actin (F-actin) are crucial for many cellular processes, including cell locomotion and cytokinesis, but are poorly understood. To define the basic principles governing microtubule/F-actin interactions, we used dual-wavelength digital fluorescence and fluorescent speckle microscopy to analyze microtubules and F-actin labeled with spectrally distinct fluorophores in interphase Xenopus egg extracts. In the absence of microtubules, networks of F-actin bundles zippered together or exhibited serpentine gliding along the coverslip. When microtubules were nucleated from Xenopus sperm centrosomes, they were released and translocated away from the aster center. In the presence of microtubules, F-actin exhibited two distinct, microtubule-dependent motilities: rapid ( approximately 250-300 nm/s) jerking and slow ( approximately 50 nm/s), straight gliding. Microtubules remodeled the F-actin network, as F-actin jerking caused centrifugal clearing of F-actin from around aster centers. F-actin jerking occurred when F-actin bound to motile microtubules powered by cytoplasmic dynein. F-actin straight gliding occurred when F-actin bundles translocated along the microtubule lattice. These interactions required Xenopus cytosolic factors. Localization of myosin-II to F-actin suggested it may power F-actin zippering, while localization of myosin-V on microtubules suggested it could mediate interactions between microtubules and F-actin. We examine current models for cytokinesis and cell motility in light of these findings.     

Effects of magnesium on the dynamic instability of individual microtubules

We investigated the effect of magnesium ion (Mg) on the parameters of dynamic instability of individual porcine brain microtubules. Rates of elongation and rapid shortening were measured by using video-enhanced DIC light microscopy and evaluated by using computer-generated plots of microtubule length vs time. Increasing [Mg] from 0.25 to 6 mM increased the second-order association rate constant for elongation about 25% at each end. At plus ends, this resulted in a 1.5-2-fold increase in elongation rates over the tubulin concentrations explored. Rapid shortening rates were more dramatically affected by Mg. As [Mg] was increased from 0.25 to 6 mM, the average rate of rapid shortening increased about 3-fold at plus ends and 4-5-fold at minus ends. The ends had roughly equivalent average rates at low [Mg], of 30-45 microns/min. At any Mg concentration, rates of disassembly varied from one microtubule to another, and often an individual microtubule would exhibit more than one rate during a single shortening phase. Individual rates at 6 mM Mg varied from 12 to 250 microns/min. Over the concentration range explored, Mg affected the frequencies of transition from elongation to shortening and back only at minus ends. Minus ends were relatively stable at low [Mg], having 4 times the frequency of rescue than at high [Mg], and a lower frequency of catastrophe (particularly evident at low tubulin concentrations). Plus ends, surprisingly, were highly unstable at all Mg concentrations investigated, having about the same transition frequencies as did the least stable (high Mg) minus ends. Our results have implications for models of the GTP cap, again emphasizing that GTP caps cannot build up in proportion to elongation rate, and must be constrained to the tips of growing microtubules.     

Membrane/microtubule tip attachment complexes (TACs) allow the assembly dynamics of plus ends to push and pull membranes into tubulovesicular networks in interphase Xenopus egg extracts

We discovered by using high resolution video microscopy, that membranes become attached selectively to the growing plus ends of microtubules by membrane/microtubule tip attachment complexes (TACs) in interphase- arrested, undiluted, Xenopus egg extracts. Persistent plus end growth of stationary microtubules pushed the membranes into thin tubules and dragged them through the cytoplasm at the approximately 20 microns/min velocity typical of free plus ends. Membrane tubules also remained attached to plus ends when they switched to the shortening phase of dynamic instability at velocities typical of free ends, 50-60 microns/min. Over time, the membrane tubules contacted and fused with one another along their lengths, forming a polygonal network much like the distribution of ER in cells. Several components of the membrane networks formed by TACs were identified as ER by immunofluorescent staining using antibodies to ER-resident proteins. TAC motility was not inhibited by known inhibitors of microtubule motor activity, including 5 mM AMP-PNP, 250 microM orthovanadate, and ATP depletion. These results show that membrane/microtubule TACs enable polymerizing ends to push and depolymerizing ends to pull membranes into thin tubular extensions and networks at fast velocities.     

Morphology of the microtubule system in mouse kidney epithelial cells]

The cultured mouse kidney cells forming epithelial sheets were studied using an indirect immunofluorescence microscopy with antibodies against tubulin. These cells, as well as fibroblasts, were found to contain a well developed microtubular system sensitive to colcemid. The assembly of microtubules after washing out of colcemid began from one or two perinuclear centers, associated with the cilium-like structure. There were certain differences between the microtubular systems in epithelial cells and fibroblasts: 1) Microtubules in the fibroblasts penetrated the whole cytoplasm including the peripheral lamella whereas in the epithelial cells the lamellar cytoplasm was often free from microtubules. 2) The orientation of microtubules in the epithelial cells, unlike in the fibroblasts, was not correlated with the stable or active state of the cell margin. A possible role of microtubular system in the epithelial cells and fibroblasts is compared and discussed.     

Three-dimensional localization and redistribution of F-actin in higher plant mitosis and cell plate formation

The distribution of F-actin cables in dividing endosperm cells of a higher plant, Haemanthus, was visualized with the immunogold-silver-enhanced method and compared with the arrangement of immunogold-stained microtubules in the same cells. The three-dimensional distribution of F-actin cables and microtubules during mitosis and cell plate formation was analyzed using ultrathin optical sectioning of whole mounts in polarized light video microscopy. F-actin cables form a loose irregular network in the interphase cytoplasm. Much of this network remains outside of the spindle during mitosis. A few F-actin cables were detected within the spindle. Their pronounced rearrangement during mitosis appears to be related to the presence and growth of microtubule arrays. During prometaphase, actin cables located on the spindle surface and those present within the spindle tend to arrange parallel to the long axis of the spindle. Cables outside the spindle do not reorient, except those at the polar region, where they appear to be compressed by the elongating spindle. Beginning with mid-anaphase, shorter actin cables oriented in various directions accumulate at the equator. Some of them are incorporated into the phragmoplast and cell plate and are gradually fragmented as the cell plate is formed and ages. Actin cables adjacent to microtubule arrays often show a regular punctate staining pattern. Such a pattern is seldom observed in the peripheral cytoplasm, which contains few microtubules. The rearrangement of F-actin cables mimicks the behavior of spindle inclusions, such as starch grains, mitochondria, etc., implying that F-actin is redistributed passively by microtubule growth or microtubule-related transport. Thus F-actin or actomyosin-based motility does not appear to be directly involved in mitosis and cytokinesis in higher plants.