Analysis of Different Methodological Approaches to Measuring 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 m. 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 m 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 m, averaging 3.33 ± 2.43 m; the average length of centrosomal microtubules was 1.49 ± 0.82 m. Good correspondence between the data on microtubule length and arrangement obtained by different methods allows the conclusion that most of the free microtubules in Vero cells actually have a length of 2–5 m; i.e., they are much shorter than the cell radius (about 25 m). 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.     

The Dynamics of Microtubules 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 with a digital camcorder. In the cell lamella, the positive ends of individual microtubules extend and shorten at random. The histograms of rate distribution have an almost normal distribution with a mode close to 0. The maximum rate of lengthening and shortening reaches 30 and 50 m/min, respectively. The positive ends of microtubules in PtK cells were in an equilibrium state, while in murine embryonic fibroblasts and Vero cells, they were usually displaced 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 PtK 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.     

CAMSAP3-dependent microtubule dynamics regulates Golgi assembly in epithelial cells

The Golgi assembly pattern varies among cell types. In fibroblast cells, the Golgi apparatus concentrates around the centrosome that radiates microtubules; whereas in epithelial cells, whose microtubules are mainly noncentrosomal, the Golgi apparatus accumulates around the nucleus independently of centrosome. Little is known about the mechanisms behind such cell type-specific Golgi and microtubule organization. Here, we show that the microtubule minus-end binding protein Nezha/CAMSAP3 (calmodulin-regulated spectrin-associated protein 3) plays a role in translocation of Golgi vesicles in epithelial cells. This function of CAMSAP3 is supported by CG-NAP (centrosome and Golgi localized PKN-associated protein) through their binding. Depletion of either one of these proteins similarly induces fragmentation of Golgi membranes. Furthermore, we find that stathmin-dependent microtubule dynamics is graded along the radial axis of cells with highest activity at the perinuclear region, and inhibition of this gradient disrupts perinuclear distribution of the Golgi apparatus. We propose that the assembly of the Golgi apparatus in epithelial cells is induced by a multi-step process, which includes CAMSAP3-dependent Golgi vesicle clustering and graded microtubule dynamics.     

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.     

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.     

Microtubule organization and function in epithelial cells

Microtubules are essential for many aspects of polarity in multicellular organisms, ranging from the asymmetric distribution of cell-fate determinants in the one-cell embryo to the transient polarity generated in migrating fibroblasts. Epithelial cells exhibit permanent cell polarity characterized by apical and basolateral surface domains of distinct protein and lipid composition that are segregated by tight junctions. They are also endowed with a microtubule network that reflects the asymmetry of their cell surface: microtubule minus-ends face the apical- and microtubule plus-ends the basal domain. Strikingly, the formation of distinct surface domains during epithelial differentiation is accompanied by the re-organization of microtubules from a uniform array focused at the centrosome to the noncentrosomal network that aligns along the apico-basolateral polarity axis. The significance of this coincidence for epithelial morphogenesis and the signaling mechanisms that drive microtubule repolymerization in developing epithelia remain major unresolved questions that we are only beginning to address. Studies in cultured polarized epithelial cells have established that microtubules serve as tracks that facilitate targeted vesicular transport. Novel findings suggest, moreover, that microtubule-based transport promotes protein sorting, and even the generation of transport carriers in the endo- and exocytic pathways.     

Free and centrosome-attached microtubules: Quantitative analysis and modeling of two-component system

In cultivated in vitro interphase animal cells, microtubules form a network whose density is highest in the central cell area, in the region of centrosome, and decreases towards the cell periphery. Since identification of individual microtubules in the central cell area is significantly difficult and more often is impossible, there are several approaches to studying microtubules in the internal cell cytoplasm. These approaches are based on a decrease of microtubule density—both real, due to their partial depolymerization (by the action of cold temperatures or cytostatics), or apparent, due to a decrease of cell thickness (by photobleaching of preexisting microtubules and analysis of newly formed ones). In the present work, we propose a method based on the determination of optical density which allows evaluation of the state of the cytoplasmic microtubule system as a whole. The method consists of a comparison of the dependences describing changes of the microtubule optical density from the cell center to the periphery in controls and in experiments. Analysis of living cells by the proposed method has shown that the character of curves describing the decrease of optical density from the cell center to its periphery is different for various cell types; the dependence can be described both as an exponential regression (the CHO cell line) and as a linear regression (the NIH-3T3 and REF cell lines). Our previous studies have allowed the suggestion that the character of the dependence is determined by the ratio of free and centrosome-attached microtubules and by the position of their ends in the cell cytoplasm. To test this hypothesis, we considered model systems with all microtubules assumed to be in a straight orientation and divergent radially from the centrosome, but with different arrangements of plus-and minus-ends. In the model system, in which all the microtubule minus-ends are attached to the centrosome while the plus-ends are at different distances from it, the microtubule density is described by the exponential (f(x) = ae ^?bx ). Introduction of free microtubules into the system leads to a change of the character of this dependence, and the system in which the concentration of free microtubules with minus ends located at different distances from the cytoplasm is 5 times higher than that of the centrosome-attached microtubules is described by the linear regression equation (f(x) = k ^* x + b), which corresponds to the experimentally obtained dependences for 3T3 and REF cells. Thus, we believe that even in cells with a radial microtubule system, free microtubules may constitute the majority.     

Free and centrosome-attached microtubules: quantitative analysis and the modeling of two-component system

In the internal cytoplasm of interphase cells the density of microtubules is the highest in the centrosome area and decreases to the cell periphery. As a rule, the quantity of fluorescent microtubules cannot be counted up in the internal cytoplasm, but it is possible to estimate microtubules quantity using measuring of their optical density. In living 3T3 and CHO cells the microtubules optical density decreased according to different mathematical dependences that apparently reflected the differences of their microtubule system organization. To determine appropriateness that circumscribe the reduction of microtubules optical density from the centrosome region to the direction of cell margin, we modeled cell contours with the certain ratio and interposition of centrosome-attached and free microtubules in vector schedules CorelDraw program. The decrease of optical density was analyzed in MetaMorph program as it was described earlier (Smurova et al., 2002). It was shown that fluorescent microtubules optical density decreased exponentially (y = ae(-bx)) if the system joined only microtubules growing from the centrosome up to the cell margin. The curve became smoother in the case of not all radial centrosome-attached microtubules reached the margin, and adding of free microtubules into the system led to the sharp fall in optical density in the centrosome area and to its gradual decrease at the cell periphery. The increase in free microtubules quantity changed the character of the curve describing the reduction of optical density microtubule system which included free and centrosome-attached microtubules in proportions of 5 : 1 was described by the equation of linear regression (f= k . x + b). Thus, the mathematical dependence describing the microtubules distribution from the centrosome to the cell periphery, depends on the ratio of microtubules and their relative positioning in the cell volume. The data obtained using model systems have coincided with the results of experiments. The graphs which described the increase in microtubules optical density during microtubule repolymerization after nocodazole treatment, corresponded to the graphs for model cells. Thus, the method we used allows to analyze the microtubule system in the cases when the direct observation of individual microtubules is difficult.     

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.     

Interphase microtubules in cultured cells: long or short?

Presently, the question about the length of microtubules in the interphase cell became actual, since the parameters of dynamic instability of the plus end measured in vivo do not allow one to explain the rapid turnover of the long microtubule system. The problem may be solved if one of the following suppositions is assumed: either microtubules undergo rapid depolymerization from the minus end or they are on the average much shorter than it is usually considered. To check the last hypothesis, we have reconstructed microtubules using stereophotography of electron microscopic sections. Microtubules around the cell center in cultures of epithelial cells (kidney of pig embryo (PK) and bovine trachea (FBT)) and fibroblasts (MEF, primary mouse embryo fibroblasts, and L cells), as well as at the periphery of PK cells were studied. All in all, no less than 200 microtubules were found near the centrosome in each cell culture. From 2.5 to 8% microtubules were beyond the studied volume (4.0 x 5.5 x 1.5 microm). Most of microtubules in all studied cell lines were up to 1 microm and about 1/3 of them were 0.2-0.4 microm long. The mean length of microtubules surrounding the centrosome in different cell lines differed insignificantly and equalled 0.4-0.8 microm. In this case, the microtubules attached to the centrosome were on the average slightly shorter than the free ones. Thus, almost all microtubules around the centrosome are short, and the majority of those attached to it do not reach the cell periphery. A similar reconstruction of a part of the PK cell cytoplasm (10 x 35 microm) has shown that at the periphery, the mean length of microtubules is about 1.6 microm and most of them are 0.5 to 1.5 microm long. Thus, our data confirm the recent hypothesis of Vorobjev et al. (I. A. Vorobjev, T. M. Svitkina, and G. G. Borisy, J. Cell Sci. 110:2635-2645 (1997)) that most of microtubules in the cells are not connected with the centrosomes.     

Caenorhabditis elegans EFA-6 limits microtubule growth at the cell cortex

Microtubules are polymers of tubulin heterodimers that exhibit dynamic instability: periods of growth followed by periods of shrinkage. However, the molecular regulation of dynamic instability remains elusive. Here, we show that EFA-6, a cortically-localized protein, limits the growth of microtubules near the cell cortex of early embryonic cells from Caenorhabditis elegans, possibly by inducing microtubule catastrophes. Compared with wild type, embryos lacking EFA-6 had abnormally long and dense microtubules at the cell cortex, and growing microtubule plus ends resided at the cortex for up to five-fold longer. Loss of EFA-6 also caused excess centrosome separation and displacement towards the cell cortex early in mitosis, and subsequently a loss of anaphase spindle-pole oscillations and increased rates of spindle elongation. The centrosome separation phenotype was dependent on the motor protein dynein, suggesting a possible link between the modulation of microtubule dynamics at the cortex and dynein-dependent force production. EFA-6 orthologues activate ARF6-type GTPases to regulate vesicle trafficking. However, we show that only the C. elegans EFA-6 amino-terminus is both necessary and sufficient to limit microtubule growth along the cortex, and that this function is independent of ARF-6.     

Microtubule dynamics in vivo: a test of mechanisms of turnover

Clarification of the mechanism of microtubule dynamics requires an analysis of the microtubule pattern at two time points in the same cell with single fiber resolution. Single microtubule resolution was obtained by microinjection of haptenized tubulin (fluorescein-tubulin) and subsequent indirect immunofluorescence with an antifluorescein antibody. The two time points in a single cell were, first, the time of photobleaching fluorescein-tubulin, and second, the time of fixation. The pattern of fluorescence replacement in the bleached zone during this time interval revealed the relevant mechanisms. In fibroblasts, microtubule domains in the bleached zone are replaced microtubule by microtubule and not by mechanisms that affect all microtubules simultaneously. Of the models we consider, treadmilling and subunit exchange along the length do not account for this observation, but dynamic instability can since it suggests that growing and shrinking microtubules coexist. In addition, we show that the half-time for microtubule replacement is shortest at the leading edge. Dynamic instability accounts for this observation if in general microtubules do not catastrophically disassemble from the plus end, but instead have a significant probability of undergoing a transition to the growing phase before they depolymerize completely. This type of instability we call tempered rather than catastrophic because, through limited disassembly followed by regrowth, it will preferentially replace polymer domains at the ends of microtubules, thus accounting for the observation that the half-time of microtubule domain replacement is shorter with proximity to the leading edge.     

Unidirectional microtubule assembly in cell-free extracts of Spisula solidissima oocytes is regulated by subtle changes in pH

Most, if not all, microtubules in vivo grow unidirectionally from a nucleation site such as the centrosome. This organized growth of microtubules can generate and maintain the radially symmetrical array of interphase microtubules as well as the bipolar mitotic apparatus. To investigate the regulation of polarized microtubule growth, we have prepared a cell-free extract from surf clam oocytes that exhibits unidirectional microtubule assembly. Immunofluorescence microscopy was used to visualize the net assembly of microtubules onto the fast (plus)- and slow (minus)- growing ends of isolated ciliary axonemes. All detectable microtubule growth in these cytoplasmic extracts occurred at the plus (+) ends and the extent of (+) end growth was regulated by subtle changes in pH. Microtubule assembly in these crude extracts was highly favored at pH 7.3, the pH of the post-fertilization cytoplasm. In contrast, when tubulin was purified from these oocyte extracts, integral components were lost, and microtubule growth became predominantly bidirectional and was favored at acidic pH. These results indicate that cytoplasmic factors may inhibit bidirectional growth in vivo and that temporal or local changes in cytoplasmic pH may influence microtubule assembly during the cell cycle.     

The polarity protein Pard3 is required for centrosome positioning during neurulation

Microtubules are essential regulators of cell polarity, architecture and motility. The organization of the microtubule network is context-specific. In non-polarized cells, microtubules are anchored to the centrosome and form radial arrays. In most epithelial cells, microtubules are noncentrosomal, align along the apico-basal axis and the centrosome templates a cilium. It follows that cells undergoing mesenchyme-to-epithelium transitions must reorganize their microtubule network extensively, yet little is understood about how this process is orchestrated. In particular, the pathways regulating the apical positioning of the centrosome are unknown, a central question given the role of cilia in fluid propulsion, sensation and signaling. In zebrafish, neural progenitors undergo progressive epithelialization during neurulation, and thus provide a convenient in vivo cellular context in which to address this question. We demonstrate here that the microtubule cytoskeleton gradually transitions from a radial to linear organization during neurulation and that microtubules function in conjunction with the polarity protein Pard3 to mediate centrosome positioning. Pard3 depletion results in hydrocephalus, a defect often associated with abnormal cerebrospinal fluid flow that has been linked to cilia defects. These findings thus bring to focus cellular events occurring during neurulation and reveal novel molecular mechanisms implicated in centrosome positioning.     

Generation and regulation of microtubule network asymmetry to drive cell polarity

Microtubules control cell architecture by serving as a scaffold for intracellular transport, signaling, and organelle positioning. Microtubules are intrinsically polarized, and their orientation, density, and post-translational modifications both respond and contribute to cell polarity. Animal cells that can rapidly reorient their polarity axis, such as fibroblasts, immune cells, and cancer cells, contain radially organized microtubule arrays anchored at the centrosome and the Golgi apparatus, whereas stably polarized cells often acquire non-centrosomal microtubule networks attached to the cell cortex, nucleus, or other structures. Microtubule density, longevity, and post-translational modifications strongly depend on the dynamics of their plus ends. Factors controlling microtubule plus-end dynamics are often part of cortical assemblies that integrate cytoskeletal organization, cell adhesion, and secretion and are subject to microtubule-dependent feedback regulation. Finally, microtubules can mechanically contribute to cell asymmetry by promoting cell elongation, a property that might be important for cells with dense microtubule arrays growing in soft environments.     

EB3 regulates microtubule dynamics at the cell cortex and is required for myoblast elongation and fusion

During muscle differentiation, myoblasts elongate and fuse into syncytial myotubes [1]. An early event during this process is the remodeling of the microtubule cytoskeleton, involving disassembly of the centrosome and, crucially, the alignment of microtubules into a parallel array along the long axis of the cell [2-5]. To further our understanding on how microtubules support myogenic differentiation, we analyzed the role of EB1-related microtubule-plus-end-binding proteins. We demonstrate that EB3 [6] is specifically upregulated upon myogenic differentiation and that knockdown of EB3, but not that of EB1, prevents myoblast elongation and fusion into myotubes. EB3-depleted cells show disorganized microtubules and fail to stabilize polarized membrane protrusions. Using live-cell imaging, we show that EB3 is necessary for the regulation of microtubule dynamics and microtubule capture at the cell cortex. Expression of EB1/EB3 chimeras on an EB3-depletion background revealed that myoblast fusion depends on two specific amino acids in the calponin-like domain of EB3, whereas the interaction sites with Clip-170 and CLASPs are dispensable. Our results suggest that EB3-mediated microtubule regulation at the cell cortex is a crucial step during myogenic differentiation and might be a general mechanism in polarized cell elongation.     

Nocodazole, vinblastine and taxol at low concentrations affect fibroblast locomotion and saltatory movements of organelles

Microtubules (MTs) are essential for the maintenance of asymmetric cell shape and motility of fibroblasts. MTs are considered to function as rails for organelle transport to the leading edge. We investigated the relationship between the motility of Vero fibroblasts and saltatory movements of particles in their lamella Fibroblasts extended their leading edges into the experimental wound at a rate of 20+/-11 microm/h. Intracellular particles in the front parts of the polarized fibroblasts moved saltatorily mainly along the long axis of the cells. MT depolymerization induced by the nocodazole at a high concentration (1.7 microM) resulted in the inhibition of both fibroblast motility and saltatory movements of the particles. Taxol (1 microM) inhibited the fibroblast locomotion but not the saltatory movements. The saltatory movement pattern was disorganized by taxol by decreasing the portion of longitudinal saltations and consequently by increasing the part of saltations perpendicular to the cell long axis. This effect may be explained by disorganization of the MT network resulting from the inhibition of dynamic instability. To further investigate the relationships between the MT dynamics instability, saltatory movements, and fibroblast locomotion, we treated fibroblasts with microtubule drugs at low concentration (nocodazole, 170 nM; vinblastine, 50 nM; and taxol, 50 nM). All these drugs induced rapid disorganization of the saltatory movements and decreased the rate of cell locomotion. Simultaneously, the amount of acetylated (stable) MTs increased. The treatment also induced reversible changes in the actin meshwork. We suggest that decrease in the fibroblast locomotion rate in the case of MT stabilization occurred because of the appearance of numerous free MTs. Saltations along free MTs are poorly organized and, as a result, the number of organelles reaching the fibroblast leading edge decreases.     

Pushing forces drive the comet-like motility of microtubule arrays in Dictyostelium

Overexpression of dynein fragments in Dictyostelium induces the movement of the entire interphase microtubule array. Centrosomes in these cells circulate through the cytoplasm at rates between 0.4 and 2.5 microm/s and are trailed by a comet-tail like arrangement of the microtubule array. Previous work suggested that these cells use a dynein-mediated pulling mechanism to generate this dramatic movement and that similar forces are at work to maintain the interphase MTOC position in wild-type cells. In the present study, we address the nature of the forces used to produce microtubule movement. We have used a laser microbeam to sever the connection between the motile centrosomes and trailing microtubules, demonstrating that the major force for such motility results from a pushing on the microtubules. We eliminate the possibility that microtubule assembly/disassembly reactions are significant contributors to this motility and suggest that the cell cortex figures prominently in locating force-producing molecules. Our findings indicate that interphase microtubules in Dictyostelium are subject to both dynein- and kinesin-like forces and that these act in concert to maintain centrosome position in the cell and to support the radial character of the microtubule network.     

How cellular membranes can regulate microtubule network

Microtubule array in eukaryotic cells supports directed transport of various cargoes driven by motor proteins. The arrangement of microtubules in cytoplasm is not stochastic; they are organized in a certain way setting a system of coordinates for intracellular transport. Most cultured fibroblast-like cells possess a radial microtubule array with the minus ends of microtubules gathered on the centrosome and plus ends directed towards the periphery of the cell. Mechanisms that regulate the formation of radial microtubule system remain unclear. Usually centrosome works as a microtubule-organizing center; however, the radial system of microtubules can be formed without centrosome participation. At least in some cases microtubule network can be organized by dynein-dynactin complexes associated with membrane vesicles. Membrane vesicles can nucleate microtubules, anchor them and move along them. However, the role of membrane organelles in microtubule organization began to attract attention of researches only recently. It this review we summarize the data indicating that membrane organelles can organize microtubules, providing “tracks” for their subsequent transport.     

Organization and dynamics of growing microtubule plus ends during early mitosis

A stable cell line expressing EB1-green fluorescent protein was used to image growing microtubule plus ends at the G(2)/M transition. By late prophase growing ends no longer extend to the cell periphery and were not uniformly distributed around each centrosome. Growing ends were much more abundant in the area surrounding the nuclear envelope, and microtubules growing around the nucleus were 1.5 fold longer than those growing in the opposite direction. The growth of longer ends toward the nucleus did not result from a localized faster growth rate, because this rate was approximately 11 microm/min in all directions from the centrosome. Rather, microtubule ends growing toward the nucleus seemed stabilized by dynein/dynactin associated with the nuclear envelope. Injection of p50 into late prophase cells removed dynein from the nuclear envelope, reduced the density of growing ends near the nuclear envelope and resulted in a uniform distribution of growing ends from each centrosome. We suggest that the cell cycle-dependent binding of dynein/dynactin to the nuclear envelope locally stabilizes growing microtubules. Both dynein and microtubules would then be in a position to participate in nuclear envelope breakdown, as described in recent studies.