Analysis of the distribution of spindle microtubules in the diatom Fragilaria.

The spindle of the colonial diatom Fragilaria contains two distinct sets of spindle microtubules (MTs): (a) MTs comprising the central spindle, which is composed of two half-spindles interdigitated to form a region of "overlap"; (b) MTs which radiate laterally from the poles. The central spindles from 28 cells are reconstructed by tracking each MT of the central spindle through consecutive serial sections. Because the colonies of Fragilaria are flat ribbons of contiguous cells (clones), it is possible, by using single ribbons of cells, to compare reconstructed spindles at different mitotic stages with minimal intercellular variability. From these reconstructions we have determined: (a) the changes in distribution of MTs along the spindle during mitosis; (b) the change in the total number of MTs during mitosis; (c) the length of each MT (measured by the number of sections each traverses) at different mitotic stages; (d) the frequency of different classes of MTs (i.e., free, continuous, etc.); (e) the spatial arrangement of MTs from opposite poles in the overlap; (f) the approximate number of MTs, separate from the central spindle, which radiate from each spindle pole. From longitudinal sections of the central spindle, the lengths of the whole spindle, half-spindle, and overlap were measured from 80 cells at different mitotic stages. Numerous sources of error may create inaccuracies in these measurements; these problems are discussed. The central spindle at prophase consists predominantly of continuous MTs (pole to pole). Between late prophase and prometaphase, spindle length increases, and the spindle is transformed into two half-spindles (mainly polar MTs) interdigitated to form the overlap. At late anaphase-telophase, the overlap decreases concurrent with spindle elongation. Our interpretation is that the MTs of the central spindle slide past one another at both late prophase and late anaphase. These changes in MT distribution have the effect of elongating the spindle and are not involved in the poleward movement of the chromosomes. Some aspects of tracking spindle MTs, the interaction of MTs in the overlap, formation of the prophase spindle, and our interpretation of rearrangements of MTs, are discussed.     

Cross-sectional structure of the central mitotic spindle of Diatoma vulgare. Evidence for specific interactions between antiparallel microtubules

During the transition from prometaphase to metaphase, the cross- sectional area of the central spindle of Diatoma decreases by a factor of nearly two, both at the poles and at the region of overlapping microtubules (MTs) near the spindle equator. The density of spindle MT packing stays approximately constant throughout mitosis. Optical diffraction analysis of electron micrographs shows that the packing of the MTs at the poles at all stages of mitosis is similar to that expected for a two-dimensional liquid. Analysis of the region of overlap reveals more packing regularity: during prometaphase, a square packing emerges that displays sufficient organization by late metaphase to generate five orders of diffraction; during anaphase the packing in the overlap region shifts to hexagonal; at telophase, it returns to square. From the data provided by serial section reconstructions of the central spindle, it is possible to identify the polarity of almost every spindle MT, that is, to identify one pole with which the MT is associated. Near neighbor analyses of MTs in cross sections of the overlap region show that MTs prefer antiparallel near neighbors. These near neighbors are most often found at a spacing of approximately 40 nm center-to-center, while parallel near neighbors in the zone of overlap are spaced essentially at random. These results are evidence for a specific interaction between antiparallel MTs. In some sections definite bridges between MTs can be seen. Our findings show that certain necessary conditions for a sliding filament model of anaphase spindle elongation are met.     

UV-microbeam irradiations of the mitotic spindle: spindle forces and structural analysis of lesions

Mitotic PtK1 spindles were UV irradiated (285 nm) during metaphase and anaphase between the chromosomes and the pole. The irradiation, a rectangle measuring 1.4 x 5 microns parallel to the metaphase plate, severed between 90 and 100% of spindle microtubules (MTs) in the irradiated region. Changes in organization of MTs in the irradiated region were analyzed by EM serial section analysis coupled with 3-D computer reconstruction. Metaphase cells irradiated 2 to 4 microns below the spindle pole (imaged by polarization optics) lost birefringence in the irradiated region. Peripheral spindle fibers, previously curved to focus on the pole, immediately splayed outwards when severed. We demonstrate via serial section analysis that following irradiation the lesion was devoid of MTs. Within 30 s to 1 min, recovery in live cells commenced as the severed spindle pole moved toward the metaphase plate closing the lesion. This movement was concomitant with the recovery of spindle birefringence and some of the severed fibers becoming refocused at the pole. Ultrastructurally we confirmed that this movement coincided with bridging of the lesion by MTs presumably growing from the pole. The non-irradiated half spindle also lost some birefringence and shortened until it resembled the recovered half spindle. Anaphase cells similarly irradiated did not show recovery of birefringence, and the pole remained disconnected from the remaining mitotic apparatus. Reconstructions of spindle structure confirmed that there were no MTs in the lesion which bridged the severed spindle pole with the remaining mitotic apparatus. These results suggest the existence of chromosome-to-pole spindle forces are dependent upon the existence of a MT continuum, and to a lesser extent to the loss of MT initiation capacity of the centrosome at the metaphase/anaphase transition.     

Quantitative analysis of an anaphase B switch: predicted role for a microtubule catastrophe gradient

Anaphase B in Drosophila embryos is initiated by the inhibition of microtubule (MT) depolymerization at spindle poles, which allows outwardly sliding interpolar (ip) MTs to drive pole-pole separation. Using fluorescence recovery after photobleaching, we observed that MTs throughout the preanaphase B spindle are very dynamic and display complete recovery of fluorescence, but during anaphase B, MTs proximal to the poles stabilize and therefore display lower recovery than those elsewhere. Fluorescence microscopy of the MT tip tracker EB1 revealed that growing MT plus ends localize throughout the preanaphase B spindle but concentrate in the overlap region of interpolar MTs (ipMTs) at anaphase B onset. None of these changes occurred in the presence of nondegradable cyclin B. Modeling suggests that they depend on the establishment of a spatial gradient of MT plus-end catastrophe frequencies, decreasing toward the equator. The resulting redistribution of ipMT plus ends to the overlap zone, together with the suppression of minus-end depolymerization at the poles, could constitute a mechanical switch that initiates spindle elongation.     

Microtubule flux and sliding in mitotic spindles of Drosophila embryos

We proposed that spindle morphogenesis in Drosophila embryos involves progression through four transient isometric structures in which a constant spacing of the spindle poles is maintained by a balance of forces generated by multiple microtubule (MT) motors and that tipping this balance drives pole-pole separation. Here we used fluorescent speckle microscopy to evaluate the influence of MT dynamics on the isometric state that persists through metaphase and anaphase A and on pole-pole separation in anaphase B. During metaphase and anaphase A, fluorescent punctae on kinetochore and interpolar MTs flux toward the poles at 0.03 microm/s, too slow to drive chromatid-to-pole motion at 0.11 microm/s, and during anaphase B, fluorescent punctae on interpolar MTs move away from the spindle equator at the same rate as the poles, consistent with MT-MT sliding. Loss of Ncd, a candidate flux motor or brake, did not affect flux in the metaphase/anaphase A isometric state or MT sliding in anaphase B but decreased the duration of the isometric state. Our results suggest that, throughout this isometric state, an outward force exerted on the spindle poles by MT sliding motors is balanced by flux, and that suppression of flux could tip the balance of forces at the onset of anaphase B, allowing MT sliding and polymerization to push the poles apart.     

Spindle microtubule dynamics following ultraviolet-microbeam irradiations of mitotic diatoms

Lesions ("ARBs") generated in metaphase and anaphase central spindles of Hantzschia by an ultraviolet microbeam are devoid of microtubules previously present. In vivo, the poleward transverse edge of the lesion invariably loses birefringence poleward, until this segment has vanished; the loss is slow during metaphase and faster at anaphase. The other transverse edge, proximal to the overlap, remains stable until disassembly of the whole spindle. We conclude that the central spindle microtubules are not in flux during metaphase to telophase, and that depolymerization of these microtubules takes place only from the end distal to the pole, as during normal spindle disassembly. Microtubule polarity and the creation of free ends may determine which microtubules are disassembled during later mitosis and how disassembly proceeds.     

Three-dimensional structure of the central mitotic spindle of Diatoma vulgare

Central mitotic spindles in Diatoma vulgare have been investigated using serial sections and electron microscopy. Spindles at both early stages (before metaphase) and later stages of mitosis (metaphase to telophase) have been analyzed. We have used computer graphics technology to facilitate the analysis and to produce stereo images of the central spindle reconstructed in three dimensions. We find that at prometaphase, when the nuclear envelope is dissassembling, the spindle is constructed from two sets of polar microtubules (MTs) that interdigitate to form a zone of overlap. As the chromosomes become organized into the metaphase configuration, the polar MTs, the spindle, and the zone of overlap all elongate, while the number of MTs in the central spindle decreases from greater than 700 to approximately 250. Most of the tubules lost are short ones that reside near the spindle poles. The previously described decrease in the length of the zone of overlap during anaphase central spindle elongation is clearly demonstrated in stereo images. In addition, we have used our three- dimensional data to determine the lengths of the spindle MTs at various times during mitotis. The distribution of lengths is bimodal during prometaphase, but the short tubules disappear and the long tubules elongate as mitosis proceeds. The distributions of MT lengths are compared to the length distributions of MTs polymerized in vitro, and a model is presented to account for our findings about both MT length changes and microtubule movements.     

Feo, the Drosophila homolog of PRC1, is required for central-spindle formation and cytokinesis

We performed a functional analysis of fascetto (feo), a Drosophila gene that encodes a protein homologous to the Ase1p/PRC1/MAP65 conserved family of microtubule-associated proteins (MAPs). These MAPs are enriched at the spindle midzone in yeast and mammals and at the fragmoplast in plants, and are essential for the organization and function of these microtubule arrays. Here we show that the Feo protein is specifically enriched at the central-spindle midzone and that its depletion either by mutation or by RNAi results in aberrant central spindles. In Feo-depleted cells, late anaphases showed normal overlap of the antiparallel MTs at the cell equator, but telophases displayed thin MT bundles of uniform width instead of robust hourglass-shaped central spindles. These thin central spindles exhibited diffuse localizations of both the Pav and Asp proteins, suggesting that these spindles comprise improperly oriented MTs. Feo-depleted cells also displayed defects in the contractile apparatus that correlated with those in the central spindle; late anaphase cells formed regular contractile structures, but these structures did not constrict during telophase, leading to failures in cytokinesis. The phenotype of Feo-depleted telophases suggests that Feo interacts with the plus ends of central spindle MTs so as to maintain their precise interdigitation during anaphase-telophase MT elongation and antiparallel sliding.     

Density and distribution of α-bungarotoxin-binding sites in postsynaptic structures of regenerated rat skeletal muscle

The polarity of kinetochore microtubules (MTs) has been studied in lysed PtK1 cells by polymerizing hook-shaped sheets of neurotubulin onto walls of preexisting cellular MTs in a fashion that reveals their structural polarity. Three different approaches are presented here: (a) we have screened the polarity of all MTs in a given spindle cross section taken from the region between the kinetochores and the poles, (b) we have determined the polarity of kinetochore MTs are more stable to cold-treated spindles; this approach takes advantage of the fact that kinetochore MTs are more stable to cold treatment than other spindle MTs; and (c) we have tracked bundles of kinetochore MTs from the vicinity of the pole to the outer layer of the kinetochore in cold- treated cells. In an anaphase cell, 90-95% of all MTs in an area between the kinetochores and the poles are of uniform polarity with their plus ends (i.e., fast growing ends) distal to the pole. In cold- treated cells, all bundles of kinetochore MTs show the same polarity; the plus ends of the MTs are located at the kinetochores. We therefore conclude that kinetochore MTs in both metaphase and anaphase cells have the same polarity as the aster MTs in each half-spindle. These results can be interpreted in two ways: (a) virtually all MTs are initiated at the spindle poles and some of the are "captured" by matured kinetochores using an as yet unknown mechanism to bind the plus ends of existing MTs; (b) the growth of kinetochore MTs is initiated at the kinetochore in such a way that the fast growing MT end is proximal to the kinetochore. Our data are inconsistent with previous kinetochore MT polarity determinations based on growth rate measurements in vitro. These studies used drug-treated cells from which chromosomes were isolated to serve as seeds for initiation of neurotubule polymerization. It is possible that under these conditions kinetochores will initiate MTs with a polarity opposite to the one described here.     

Verteilung der Mikrotubuli in Metaphase- und Anaphase-Spindeln der Spermatocyten von Pales ferruginea

One metaphase I spindle, seven anaphase I spindles of different stages, and one metaphase II spindle were sectioned in series. The ultrastructure of chromosomes was examined and microtubules (MTs) were counted. The main results of the study are summarized as follows: 1. The autosomes move at the periphery of the continuous MTs during anaphase while the sex chromosomes move more or less within this group of MTs. 2. In metaphase the antosomes have few coarse surface projections, in anaphase many, but more delicate projections of irregular shape which seem to transform into regular radial lamellae at the end of movement. 3. In metaphase continuous MTs have no contact with the chromosomal surface, while during anaphase movement continuous MTs lie closer to the chromosomes, and finally arrange themselves between the radial surface lamellae. There they show lateral filamentous connections with the chromosomal surface. 4. The MT distribution profiles of metaphase and anaphase are different. While the highest density of MTs is observed in the middle region of the spindle in metaphase, there are two density zones during autosomal movement, each in one half spindle in front of the autosomes. After the autosomes have reached the poles the distribution profile is again similar to the metaphase condition. The MT distribution in metaphase II is the same as in metaphase I. Possible explanations for these observations are discussed in detail. 5. There is an overall decrease in MT content during anaphase. 6. With the onset of anaphase MTs are seen within the spindle mantle, closely associated with mitochondria. — Several theoretical aspects of anaphase mechanism are briefly discussed.     

Reverse engineering of force integration during mitosis in the Drosophila embryo

The mitotic spindle is a complex macromolecular machine that coordinates accurate chromosome segregation. The spindle accomplishes its function using forces generated by microtubules (MTs) and multiple molecular motors, but how these forces are integrated remains unclear, since the temporal activation profiles and the mechanical characteristics of the relevant motors are largely unknown. Here, we developed a computational search algorithm that uses experimental measurements to ‘reverse engineer’ molecular mechanical machines. Our algorithm uses measurements of length time series for wild‐type and experimentally perturbed spindles to identify mechanistic models for coordination of the mitotic force generators in Drosophila embryo spindles. The search eliminated thousands of possible models and identified six distinct strategies for MT–motor integration that agree with available data. Many features of these six predicted strategies are conserved, including a persistent kinesin‐5‐driven sliding filament mechanism combined with the anaphase B‐specific inhibition of a kinesin‐13 MT depolymerase on spindle poles. Such conserved features allow predictions of force–velocity characteristics and activation–deactivation profiles of key mitotic motors. Identified differences among the six predicted strategies regarding the mechanisms of prometaphase and anaphase spindle elongation suggest future experiments.     

The mechanism of anaphase spindle elongation

At anaphase chromosomes move to the spindle poles (anaphase A) and the spindle poles move apart (anaphase B). In vitro studies using isolated diatom spindles demonstrate that the primary mechanochemical event responsible for spindle elongation is the sliding apart of half-spindle microtubules. Further, these forces are generated within the zone of microtubule overlap in the spindle mid-zone.     

The microtubule-based motor Kar3 and plus end-binding protein Bim1 provide structural support for the anaphase spindle

In budding yeast, the mitotic spindle is comprised of 32 kinetochore microtubules (kMTs) and ~8 interpolar MTs (ipMTs). Upon anaphase onset, kMTs shorten to the pole, whereas ipMTs increase in length. Overlapping MTs are responsible for the maintenance of spindle integrity during anaphase. To dissect the requirements for anaphase spindle stability, we introduced a conditionally functional dicentric chromosome into yeast. When centromeres from the same sister chromatid attach to opposite poles, anaphase spindle elongation is delayed and a DNA breakage-fusion-bridge cycle ensues that is dependent on DNA repair proteins. We find that cell survival after dicentric chromosome activation requires the MT-binding proteins Kar3p, Bim1p, and Ase1p. In their absence, anaphase spindles are prone to collapse and buckle in the presence of a dicentric chromosome. Our analysis reveals the importance of Bim1p in maintaining a stable ipMT overlap zone by promoting polymerization of ipMTs during anaphase, whereas Kar3p contributes to spindle stability by cross-linking spindle MTs.     

Mechanism for Anaphase B: Evaluation of “Slide-and-Cluster” versus “Slide-and-Flux-or-Elongate” Models

Elongation of the mitotic spindle during anaphase B contributes to chromosome segregation in many cells. Here, we quantitatively test the ability of two models for spindle length control to describe the dynamics of anaphase B spindle elongation using experimental data from Drosophila embryos. In the slide-and-flux-or-elongate (SAFE) model, kinesin-5 motors persistently slide apart antiparallel interpolar microtubules (ipMTs). During pre-anaphase B, this outward sliding of ipMTs is balanced by depolymerization of their minus ends at the poles, producing poleward flux, while the spindle maintains a constant length. Following cyclin B degradation, ipMT depolymerization ceases so the sliding ipMTs can push the poles apart. The competing slide-and-cluster (SAC) model proposes that MTs nucleated at the equator are slid outward by the cooperative actions of the bipolar kinesin-5 and a minus-end-directed motor, which then pulls the sliding MTs inward and clusters them at the poles. In assessing both models, we assume that kinesin-5 preferentially cross-links and slides apart antiparallel MTs while the MT plus ends exhibit dynamic instability. However, in the SAC model, minus-end-directed motors bind the minus ends of MTs as cargo and transport them poleward along adjacent, parallel MT tracks, whereas in the SAFE model, all MT minus ends that reach the pole are depolymerized by kinesin-13. Remarkably, the results show that within a narrow range of MT dynamic instability parameters, both models can reproduce the steady-state length and dynamics of pre-anaphase B spindles and the rate of anaphase B spindle elongation. However, only the SAFE model reproduces the change in MT dynamics observed experimentally at anaphase B onset. Thus, although both models explain many features of anaphase B in this system, our quantitative evaluation of experimental data regarding several different aspects of spindle dynamics suggests that the SAFE model provides a better fit.     

Functional central spindle assembly requires de novo microtubule generation in the interchromosomal region during anaphase

The central spindle forms between segregating chromosomes during anaphase and is required for cytokinesis. Although anaphase-specific bundling and stabilization of interpolar microtubules (MTs) contribute to formation of the central spindle, it remains largely unknown how these MTs are prepared. Using live imaging of MT plus ends and an MT depolymerization and regrowth assay, we show that de novo MT generation in the interchromosomal region during anaphase is important for central spindle formation in human cells. Generation of interchromosomal MTs and subsequent formation of the central spindle occur independently of preanaphase MTs or centrosomal MT nucleation but require augmin, a protein complex implicated in nucleation of noncentrosomal MTs during preanaphase. MTs generated in a hepatoma up-regulated protein (HURP)-dependent manner during anaphase also contribute to central spindle formation redundantly with preanaphase MTs. Based on these results, a new model for central spindle assembly is proposed.     

Microtubule dynamics in the spindle. Theoretical aspects of assembly/disassembly reactions in vivo

The mitotic spindle contains several classes of microtubules (MTs) whose lengths change independently during mitosis. Precise control over MT polymerization and depolymerization during spindle formation, anaphase chromosome movements, and spindle breakdown is necessary for successful cell division. This model proposes the site of addition and removal of MT subunits in each of four classes of spindle MTs at different stages of mitosis, and suggests how this addition and removal is controlled. We propose that spindle poles and kinetochores significantly alter the assembly-disassembly kinetics of associated MT ends. Control of MT length is further modulated by localized forces affecting assembly and disassembly kinetics of individual sets of MTs.     

Laser microsurgery in fission yeast; role of the mitotic spindle midzone in anaphase B

INTRODUCTION: During anaphase B in mitosis, polymerization and sliding of overlapping spindle microtubules (MTs) contribute to the outward movement the spindle pole bodies (SPBs). To probe the mechanism of spindle elongation, we combine fluorescence microscopy, photobleaching, and laser microsurgery in the fission yeast Schizosaccharomyces pombe. RESULTS: We demonstrate that a green laser cuts intracellular structures in yeast cells with high spatial specificity. By using laser microsurgery, we cut mitotic spindles labeled with GFP-tubulin at various stages of anaphase B. Although cutting generally caused early anaphase spindles to disassemble, midanaphase spindle fragments continued to elongate. In particular, when the spindle was cut near a SPB, the larger spindle fragment continued to elongate in the direction of the cut. Photobleach marks showed that sliding of overlapping midzone MTs was responsible for the elongation of the spindle fragment. Spindle midzone fragments not connected to either of the two spindle poles also elongated. Equatorial microtubule organizing center (eMTOC) activity was not affected in cells with one detached pole but was delayed or absent in cells with two detached poles. CONCLUSIONS: These studies reveal that the spindle midzone is necessary and sufficient for the stabilization of MT ends and for spindle elongation. By contrast, SPBs are not required for elongation, but they contribute to the attachment of the nuclear envelope and chromosomes to the spindle, and to cell cycle progression. Laser microsurgery provides a means by which to dissect the mechanics of the spindle in yeast.     

Self-organization of anastral spindles by synergy of dynamic instability, autocatalytic microtubule production, and a spatial signaling gradient

Assembly of the mitotic spindle is a classic example of macromolecular self-organization. During spindle assembly, microtubules (MTs) accumulate around chromatin. In centrosomal spindles, centrosomes at the spindle poles are the dominating source of MT production. However, many systems assemble anastral spindles, i.e., spindles without centrosomes at the poles. How anastral spindles produce and maintain a high concentration of MTs in the absence of centrosome-catalyzed MT production is unknown. With a combined biochemistry-computer simulation approach, we show that the concerted activity of three components can efficiently concentrate microtubules (MTs) at chromatin: (1) an external stimulus in form of a RanGTP gradient centered on chromatin, (2) a feed-back loop where MTs induce production of new MTs, and (3) continuous re-organization of MT structures by dynamic instability. The mechanism proposed here can generate and maintain a dissipative MT super-structure within a RanGTP gradient.     

Microtubule organization and distribution of gamma-tubulin in male meiosis of lepidoptera

Meiotic spindles in males of higher Lepidotera are unusual in that the bulk of the spindle microtubules (MTs) ends about halfway between the equatorial plate and the centrosomes in metaphase. It appears worthwhile to determine how the MTs are nucleated, while their pole proximal ends are distant from the centrosomes. To this end, spermatocytes of Phragmatobia fuliginosa (Arctiidae), collected in the field, were double-labeled with antibodies to beta- and gamma-tubulin. The former antibody reveals the entire microtubular cytoskeleton, and the latter is directed against a newly-discovered tublin isoform that is prevalent in microtubule-organizing centers (MTOCs). The immunocytochemical work was supplemented by a fine structural analysis of MTOCs and spindles. Gamma-tubulin was clearly detected at the spindle poles, and prominent microtubular asters originated from these sites. Additionally, MT arrays at both sides of the equatorial plate in metaphase spermatocytes contained gamma-tubulin. The staining persisted in late anaphase, when kinetochore MTs are depolymerized. This indicates that at least nonkinetochore MTs contain gamma-tubulin. The analysis of ultrathin sections through spindles revealed large amounts of pericentriolar material at the spindles poles, in prometaphase through anaphase. The spindle MTs appeared as regular, straight elements in longitudinal sections. We assume that gamma-tubulin is located at the pole proximal ends of the MTs and/or is associated with the spindle MTs throughout their lengths. In order to distinguish between these possibilities, testes of Ephestia kuehniella (Pyralidae), a laboratory species, were cold-treated prior to double-labeling with antibodies to beta- and gamma-tubulin. The treatment was expected to depolymerize MTs. Astral MTs, which were nucleated end-on by gamma-tubulin-containing material, indeed depolymerized. In contrast, the gamma-tubulin-containing spindle MTs persisted. It is, therefore, conceivable that gamma-tubulin is associated with MTs throughout their lengths in male meiosis of Lepidoptera species. It is plausible that this association stabilizes the MTs against cold-induced disassembly. © 1996 Wiley-Liss, Inc.     

Cell division and nuclear movement in the saccoderm desmidNetrium interruptus

Summary During anaphase in thisNetrium, the reforming daughter nuclei hardly pause at the poles before they elongate and rapidly and smoothly move along the daughter cells in one of the grooves in the chloroplast. Ahead of each nucleus is a pointed mass of cytoplasm that is distinctly striated; straight, mobile strands of cytoplasm emanate from this region ahead of the nucleus. When the nucleus reaches the large vacuole that divides the two chloroplasts, it steadily slides over to the chloroplast surface distal to the cleavage furrow. It then stops moving and slowly expands into the normal interphase morphology.Under the electron microscope, the chromosome-to-pole distance does not decrease much during anaphase (i.e., anaphase A is minimal) and so the half spindles remain about the same length by telophase. The poles of the open spindle are initially broad and contain typical spindle microtubules (MTs). These persist intact during anaphase and become focused upon a discrete Organizing Centre as the daughter nuclei reform. These MTs become a cone-shaped array that creates the pointed cytoplasmic mass ahead of the moving nucleus in live cells. Thus, this placoderm desmid behaves very likeClosterium during division and shows the lack of anaphase A, and the transformation of the telophase spindle into a MT-based motility system, now characteristic of many members of the Zygnematales.Abbreviations MT microtubule - MTOC microtubule organizing centre Dedicated to the memory of Professor Oswald Kiermayer