Structure–property relation and relevance of beam theories for microtubules: a coupled molecular and continuum mechanics study

Quasi-one-dimensional microtubules (MTs) in cells enjoy high axial rigidity but large transverse flexibility due to the inter-protofilament (PF) sliding. This study aims to explore the structure–property relation for MTs and examine the relevance of the beam theories to their unique features. A molecular structural mechanics (MSM) model was used to identify the origin of the inter-PF sliding and its role in bending and vibration of MTs. The beam models were then fitted to the MSM to reveal how they cope with the distinct mechanical responses induced by the inter-PF sliding. Clear evidence showed that the inter-PF sliding is due to the soft inter-PF bonds and leads to the length-dependent bending stiffness. The Euler beam theory is found to adequately describe MT deformation when the inter-PF sliding is largely prohibited. Nevertheless, neither shear deformation nor the nonlocal effect considered in the ‘more accurate’ beam theories can fully capture the effect of the inter-PF sliding. This reflects the distinct deformation mechanisms between an MT and its equivalent continuous body.     

Molecular investigation of the mechanical properties of single actin filaments based on vibration analyses

The mechanical vibration properties of single actin filaments from 50 to 288 nm are investigated by the molecular dynamics simulation in this study. The natural frequencies obtained from the molecular simulations agree with those obtained from the analytical solution of the equivalent Euler–Bernoulli beam model. Through the convergence study of the mechanical properties with respect to the filament length, it was found that the Euler–Bernoulli beam model can only be reliably used when the single actin filament is of the order of hundreds of nanometre scale. This molecular investigation not only provides the evidence for the use of the continuum beam model in characterising the mechanical properties of single actin filaments, but also clarifies the criteria for the effective use of the Euler–Bernoulli beam model.     

How the transition frequencies of microtubule dynamic instability (nucleation, catastrophe, and rescue) regulate microtubule dynamics in interphase and mitosis: analysis using a Monte Carlo computer simulation.

Microtubules (MTs) in newt mitotic spindles grow faster than MTs in the interphase cytoplasmic microtubule complex (CMTC), yet spindle MTs do not have the long lengths or lifetimes of the CMTC microtubules. Because MTs undergo dynamic instability, it is likely that changes in the durations of growth or shortening are responsible for this anomaly. We have used a Monte Carlo computer simulation to examine how changes in the number of MTs and changes in the catastrophe and rescue frequencies of dynamic instability may be responsible for the cell cycle dependent changes in MT characteristics. We used the computer simulations to model interphase-like or mitotic-like MT populations on the basis of the dynamic instability parameters available from newt lung epithelial cells in vivo. We started with parameters that produced MT populations similar to the interphase newt lung cell CMTC. In the simulation, increasing the number of MTs and either increasing the frequency of catastrophe or decreasing the frequency of rescue reproduced the changes in MT dynamics measured in vivo between interphase and mitosis.     

Polarized transport of Frizzled along the planar microtubule arrays in Drosophila wing epithelium

Cells in a variety of developmental contexts sense extracellular cues that are given locally on their surfaces, and subsequently amplify the initial signal to achieve cell polarization. Drosophila wing cells acquire planar polarity along the proximal-distal (P-D) axis, in which the amplification of the presumptive cue involves assembly of a multiprotein complex that spans distal and proximal boundaries of adjacent cells. Here we pursue the mechanisms that place one of the components, Frizzled (Fz), at the distal side. Intracellular particles of GFP-tagged Fz moved preferentially toward distal boundaries before Fz::GFP and other components were tightly localized at the P/D cortex. Arrays of microtubules (MTs) were approximately oriented along the P-D axis and these MTs contributed to the formation of the cortical complex. Furthermore, there appeared to be a bias in the P-D MTs, with slightly more plus ends oriented distally. The hypothesis of polarized vesicular trafficking of Fz is discussed.     

Dynamics of microtubule reassembly and reorganization in the coenocytic green alga Ernodesmis verticillata (Kützing) Børgesen

The dynamics of microtubule (MT) disassembly and reassembly were studied in the green alga Ernodesmis verticillata, using indirect immunofluorescent localization of tubulin. This alga possesses two distinct MT arrays: highly-ordered, longitudinally-oriented cortical MTs, and shorter perinuclear MTs radiating from nuclear surfaces. Perinuclear MTs are very labile, completely disassembling in the cold (cells on ice) within 5–10 min or in 25 μM amiprophos-methyl (APM) within 15–30 min. Although cortical MTs are generally absent after 3 h in APM, it takes 45–60 min before any cold-induced depolymerization is apparent, and some cortical MTs persist after 6 h of cold treatment. The extent of immunofluorescence of cytoplasmic (depolymerized?) tubulin is inversely proportional to the abundance of cortical MTs. Recovery of MT arrays upon warming or upon removal of APM occurs within 30–60 min for the perinuclear MTs, but the cortical arrays take much longer to regain their normal patterns. The cortical MTs initially reappear in a random distribution with respect to the cell axis, but within 3–4 d of warming (or 24–36 h of removing APM) they are nearly parallel to each other and to the cell's longitudinal axis. Thus, although the timing differs, the actual patterns of depolymerization and recovery are similar, irrespective of whether physical or chemical agents are used. Longer-term treatments in 1 μM APM indicate that despite the rapid disappearance of perinuclear MTs, a loss of the uniform nuclear spacing occurs gradually over 1–6 d. Similar disorganization of nuclei is obtained with long-term treatment with 1 μM taxol, where a gradual loss of perinuclear MTs is accompanied by an increased abundance of mitotic spindles. This implies that perinuclear MTs can disassemble in vivo in the presence of taxol, and that they are not the sole components involved in maintaining nuclear spacing in these coenocytes. The results indicate that both nuclear and cortical sites of MT nucleation may exist in this organism, and that MT reassembly and re-organization are temporally distinct events in cells that have highly-ordered arrays of long MTs.     

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.     

Ultrastructural Observation on Microtubules of the Generative Cell in Amaryllis Germinated Pollens and Pollen Tubes

The organization of microtubules (MTs) in the generative cell (GC) of germinated pollen and pollen tube in Amaryllis vittata Ait. has been studied with electron microscopy. At the beginning of pollen germination, the GC is long elliptic in shape, and is surrounded by its own membrane and also by that of the vegetative cell (VC) ,both of which appear undulated. In cross section, the GC appears roundish and has many lobes. The MT system of GC is mainly organized in bundles, but single MTs can also be observed. The MT bundles are generally located in the lobes, directly beneath the plasma membrane of the cell. These MT bundles orientate along the longitudinal axis of the cell. They are formed by aggregation of 5–6 MTs at least,more often about 30 MTs. In the bundles the MTs are often linked to each other by "cross-bridge". The single tubules in the eytopiasm distribute randomly in different orientations. When the GC has migrated into the pollen tube after germination ,it becomes elongated and has cytoplasmic extensions both in the anterior and posterior end of the cell. The organization of MTs of the GC in pollen tube is similar to that in the germinated pollen grain,but the number of MTs in a bundle often increases to 50–60. In the bundle the "cross-bridges" between the MTs which always link 3–5 MTs, are still seen clearly. Positional shift between the GC and Vegetative nucleus (VN) may take place during the growth of pollen tube. The physical association between GC and VN may be demonstrated some ultrastructural figures. It may be seen that irregular cytoplasmic extensions in the anterior end of the GC is always enclosed by the VN and the projections of the cytoplasmic extensions lie within enclaves of the VN. There are many MTs sheets in the lobes or extensions in the cytoplasm of the GC. Thus the present study demonstrates that MTs have an important role in maintaining the peculiar shape of the GC and the close association between GC and VN. However, it seems that the MTs are probably also engaged in the movement of the GC during pollen growth.     

Colocalization studies of Arp1 and p150Glued to spindle microtubules during mitosis: the effect of cytochalasin on the organization of microtubules and motor proteins in PtK1 cells

Motor proteins play a fundamental role in the congression and segregation of chromosomes in mitosis as well as the formation of the mitotic spindle. In particular, the dynein/dynactin complex is involved in the maintenance of the spindle, formation of astral microtubules, chromosome motion, and chromosome segregation. Dynactin is a multisubunit, high molecular weight protein that is responsible for the attachment of cargo to dynein. There are a number of major subunits in dynactin that are presumed to be important during mitosis. Arp1 is thought to be the attachment site for cargo to the complex while p150(Glued), a side arm of this complex regulates binding to MTs and the binding of dynactin to dynein. We performed colocalization studies of Arp1 and p150(Glued) to spindle microtubules. Both Arp1 and p150(Glued) colocalize with spindle MTs as well as cytoplasmic components. When treated with cytochalasin J, Arp1 concentrates at the centrosomes and is less co-localized with spindle MTs. Cytochalasin J has less of an effect on the colocalization of p150(Glued) with spindle MTs, suggesting that Arp1 may have a cytochalasin J sensitive site.     

Dynamics of spindle microtubule organization: kinetochore fiber microtubules of plant endosperm

Organization of kinetochore fiber microtubules (MTs) throughout mitosis in the endosperm of Haemanthus katherinae Bak. has been analysed using serial section reconstruction from electron micrographs. Accurate and complete studies have required careful analysis of individual MTs in precisely oriented serial sections through many (45) preselected cells. Kinetochore MTs (kMTs) and non-kinetochore MTs (nkMTs) intermingle within the fiber throughout division, undergoing characteristic, time- dependent, organizational changes. The number of kMTs increases progressively throughout the kinetochore during prometaphase-metaphase. Prometaphase chromosomes which were probably moving toward the pole at the time of fixation have unequally developed kinetochores associated with many nkMTs. The greatest numbers of kMTs (74-109/kinetochore), kinetochore cross-sectional area, and kMT central density all occur at metaphase. Throughout anaphase and telophase there is a decrease in the number of kMTs and, in the kinetochore cross-sectional area, an increased obliquity of kMTs and increased numbers of short MTs near the kinetochore. Delayed kinetochores possess more kMTs than do kinetochores near the poles, but fewer kMTs than chromosomes which have moved equivalent distances in other cells. The frequency of C-shaped proximal MT terminations within kinetochores is highest at early prometaphase and midtelophase, falling to zero at midanaphase. Therefore, in Haemanthus, MTs are probably lost from the periphery of the kinetochore during anaphase in a manner which is related to both time and position of the chromosome along the spindle axis. The complex, time-dependent organization of MTs in the kinetochore region strongly suggests that chromosome movement is accompanied by continual MT rearrangement and/or assembly/disassembly.     

Circumferential vibration of microtubules with long axial wavelength

This paper uses an orthotropic shell model to investigate in detail the long axial wavelength circumferential vibration of microtubules (MTs). The deformation patterns in the vibrations were explored and their phonon dispersion relations were presented for MTs with increasing radius. It was shown that with the growth of the axial wavelength, the associated frequency of MTs would finally approach a nonzero asymptotic value, rising considerably with the increase of circumferential wave number but dropping linearly with the growing radius. This study corrects the previous misunderstanding drawn by an oversimplified model, and points out that a parabolic dispersion law does not apply to the circumferential modes when the MT bending stiffness is properly considered.     

Dynamics and the life cycle of cell microtubules

In living cells microtubules (MTs) continuously grow and shorten. This feature of MTs was discovered in vitro and named dynamic instability. Comparison of dynamic instability of MTs in vitro and in vivo shows a number of differences. MTs in vivo rapidly grow (up to 20 microns/min), duration of their shortening is small (on average 15-20 s), and pauses are prominent. In different animal cells MTs grow from the centrosome and form a radial array. In such cells growth of MTs is persistent, i.e. undergo without interruptions until plus end of a MT reaches cell margin. Analysis of literature and original data shows that interconvertion between phases of growth, shortening and pause is asymmetric: growth often converts into pause, while shortening always converts into growth without pause. We suggest dynamic instability described near the cell margin in numerous publications results not only from intrinsic properties of MTs, but also because of the external obstacles for their growth. MT behavior in the cells with radial array of long MTs could be treated as dynamic instability with boundary conditions. One boundary is the centrosome responsible for rapid initiation of MT growth. Another boundary is cell margin limiting MT elongation. MT growth occurs with constant mean velocity, and potential duration of growth phase might exceed cell radius. MT shortening is usually smaller than MT length however velocity of shortening increases with time. Random episodes of rapid shortening are sufficient for the exchange of MTs in 10-20 min in the cells not more than 40-50 microns in diameter. Experimental data show that similar rate of exchange of MTs is in the large cells. This is achieved employing another mechanism, namely release of MTs and depolymerization from the minus end. In the minus end pathway time required for the exchange of MTs does not depend on cell radius and is determined primarily by the frequency of releases. Thus a small number of free MTs with metastable minus ends significantly reduce time required for the renovation of the radial MT array. Summarizing all experimental data we suggest the life cycle scheme for the MT in a cell. MT is initiated at the centrosome and grows rapidly until it reaches cell margin. At the margin the plus end oscillates, and finally MT depolimerizes. MT "death" comes from a random catastrophe (shortening from the plus end) in small cells or from release and depolymerization of the minus end in large cells.     

Effects of the cross-linkers on the buckling of microtubules in cells

In cells, the protein cross-linkers lead to a distinct buckling behavior of microtubules (MTs) different from the buckling of individual MTs. This paper thus aims to examine this issue via the molecular structural mechanics (MSM) simulations. The transition of buckling responses was captured as the two-dimensional-linkers were replaced by the three-dimensional (3D) ones. Then, the effects of the radial orientation and the axial density of the 3D-linkers were examined, showing that more uniform distribution of the radial orientation leads to the higher critical load with 3D buckling modes, while the inhomogeneity of the axial density results in the localized buckling patterns. The results demonstrated the important role of the cross-linker in regulating MT stiffness, revealed the physics of the experimentally observed localized buckling and these results will pave the way to a new multi-component mechanics model for whole cells.     

Structural and functional diversity in the neuronal microtubules of Caenorhabditis elegans

Tannic acid fixation reveals differences in the number of protofilaments between microtubules (MTs) in the nematode Caenorhabditis elegans. Most cells have MTs with 11 protofilaments but the six touch receptor neurons (the microtubule cells) have MTs with 15 protofilaments. No 13-protofilament (13-p) MT has been seen. The modified cilia of sensory neurons also possess unusual structures. The cilia contain nine outer doublets with A subfibers of 13 protofilaments and B subfibers of 11 protofilaments and a variable number of inner singlet MTs containing 11 protofilaments. The 15-p MTs but not the 11-p MTs are eliminated by colchicine-treatment or by mutation of the gene mec-7. Concomitantly, touch sensitivity is also lost. However, whereas colchicine treatment leads to the loss of all MTs from the microtubule cells, mutations in mec-7 result in the partial replacement of the 15-p MTs with 11-p MTs. Benzimidazoles (benomyl and nocodazole) have more general effects on C. elegans (slow growth, severe uncoordination, and loss of processes from the ventral cord) but do not affect the 15-p MTs. Benomyl will, however, disrupt the replacement 11-p MTs found in the microtubule cells of mec-7 mutants. The 11-p and 15-p MTs also respond differently to temperature and fixation conditions. It is likely that either type of MT will suffice for the proper outgrowth of the microtubule cell process, but only the 15-p MT can function in the specialized role of sensory transduction of the microtubule cells.     

Beamline characterization of a dielectric-filled reentrant cavity resonator as beam current monitor for a medical cyclotron facility

At PSI (Paul Scherrer Institute), Switzerland, a superconducting cyclotron called “COMET” delivers proton beam of 250 MeV pulsed at 72.85 MHz for proton radiation therapy. Measuring proton beam currents (0.1–10nA) is of crucial importance for the treatment safety and is usually performed with invasive monitors such as ionisation chambers (ICs) which degrade the beam quality. A new non-invasive beam current monitor working on the principle of electromagnetic resonance is built to replace ICs in order to preserve the beam quality delivered. The fundamental resonance frequency of the resonator is tuned to 145.7 MHz, which is the second harmonic of the pulse rate, so it provides signals proportional to beam current. The cavity resonator installed in the beamline of the COMET is designed to measure beam currents for the energy range 238–70 MeV. Good agreement is reached between expected and measured resonator response over the energy range of interest. The resonator can deliver beam current information down to 0.15 nA for a measurement integration time of 1 s. The cavity resonator might be applied serving as a safety monitor to trigger interlocks within the existing domain of proton radiation therapy. Low beam currents limit the abilities to detect sufficiently, however, with the potential implementation of FLASH proton therapy, the application of cavity resonator as an online beam-monitoring device is feasible.     

Wire tension versus wire frequency: An experimental Ilizarov frame study

Stability of an Ilizarov frame highly depends on maintenance of adequate tension in the wires. Wire tension should be measured accurately in experimental laboratory studies when new types of wire fixators are tested. In this study, 20 wires were tested using two different wire fixators. The wires were sequentially tensioned from 0 to 1275 N in 50 N intervals. For each tension value, corresponding vibration frequency was recorded. We then described the relationship between wire tension and wire vibration frequency in an empirical equation (R²=99.8). Wire vibration frequency can also be described theoretically by the Euler–Bernoulli equation for a thin beam. Theoretical frequencies were calculated and compared with corresponding experimental frequencies. A close agreement was found (95% limits of agreement, ±3.2 Hz). This empirical equation represents a simple tool, applicable when investigating the effect of new wire fixators, pre-tensioning and frame constructions on wire tension.     

HIV Transmission among Men Who Have Sex with Men due to Condom Failure

Background

Despite preventive efforts, HIV incidence remains high among men who have sex with men (MSM) in industrialized countries. Condoms are an important element in prevention but, given the high frequency of condom use and their imperfect effectiveness, a substantial number and proportion of HIV transmissions may occur despite condoms. We developed a model to examine this hypothesis.

Methods

We used estimates of annual prevalent and incident HIV infections for MSM in Ontario. For HIV-negative men, we applied frequencies of sexual episodes and per-contact HIV transmission risks of receptive and insertive anal sex with and without a condom and oral sex without a condom. We factored in the proportion of HIV-infected partners receiving antiretroviral therapy and its impact in reducing transmissibility. We used Monte-Carlo simulation to determine the plausible range for the proportion of HIV transmissions for each sexual practice.

Results

Among Ontario MSM in 2009, an estimated 92,963 HIV-negative men had 1,184,343 episodes of anal sex with a condom and 117,133 anal sex acts without a condom with an HIV-positive partner. Of the 693 new HIV infections, 51% were through anal sex with a condom, 33% anal sex without a condom and 16% oral sex. For anal sex with a condom, the 95% confidence limits were 17% and 77%.

Conclusions

The proportion of HIV infections related to condom failure appears substantial and higher than previously thought. That 51% of transmissions occur despite condom use may be conservative (i.e. low) since we used a relatively high estimate (87.1%) for condom effectiveness. If condom effectiveness were closer to 70%, a value estimated from a recent CDC study, the number and proportion of HIV transmissions occurring despite condom use would be much higher. Therefore, while condom use should continue to be promoted and enhanced, this alone is unlikely to stem the tide of HIV infection among MSM.     

Three-dimensional reconstruction and analysis of mitotic spindles from the yeast, Schizosaccharomyces pombe

Mitotic spindles of Schizosaccharomyces pombe have been studied by EM, using serial cross sections to reconstruct 12 spindles from cells that were ultrarapidly frozen and fixed by freeze substitution. The resulting distributions of microtubules (MTs) have been analyzed by computer. Short spindles contain two kinds of MTs: continuous ones that run from pole to pole and MTs that originate at one pole and end in the body of the spindle. Among the latter there are three pairs of MT bundles that end on fibrous, darkly staining structures that we interpret as kinetochores. The number of MTs ending at each putative kinetochore ranges from two to four; all kinetochore-associated MTs disappear as the spindle elongates from 3-6 microns. At this and greater spindle lengths, there are no continuous MTs, only polar MTs that interdigitate at the spindle midzone, but the spindle continues to elongate. An analysis of the density of neighboring MTs at the midzone of long spindles shows that their most common spacing is approximately 40 nm, center to center, and that there is a preferred angular separation of 90 degrees. Only hints of such square-packing are found at the midzone of short spindles, and near the poles there is no apparent order at any mitotic stage. Our data suggest that the kinetochore MTs (KMTs) do not interact directly with nonkinetochore MTs, but that interdigitating MTs from the two spindle poles do interact to form a mechanically stable bundle that connects the poles. As the spindle elongates, the number of MTs decreases while the mean length of the MTs that remain increases. We conclude that the chromosomes of S. pombe become attached to the spindle by kinetochore MTs, that these MTs disappear as the chromosomes segregate, that increased separation of daughter nuclei is accompanied by a sliding apart of anti-parallel MTs, and that the mitotic processes of S. pombe are much like those in other eukaryotic cells.     

Processes induced by tau expression in Sf9 cells have an axon-like microtubule organization

We have indirectly analyzed the role of tau in generating the highly organized microtubule (MT) array of the axon. Axons contain MT arrays of uniform polarity orientation, plus ends distal to the cell body (Heidemann, S. R., J. M. Landers, and M. A. Hamborg. 1981. J. Cell Biol. 91:661-673). Surprisingly, these MTs do not radiate from a single discrete nucleating structure in the cell body (Sharp, G. A., K. Weber, and M. Osborn. 1982. Eur. J. Cell Biol. 29: 97-103), but rather stop and start at multiple sites along the length of the axon (Bray, D., and M. B. Bunge. 1981. J. Neurocytol. 10:589-605). When Sf9 ovarian cells are induced to express high levels of tau protein, they develop cellular processes which are similar in appearance to axons and which contain dense arrays of MTs (Knops, J., K. S. Kosik, G. Lee, J. D. Pardee, L. Cohen-Gould, and L. McConlogue. 1991. J. Cell Biol. 114:725-734). We have analyzed the organization of MTs within these arrays, and determined it to be similar, but not identical, to the organization of MTs within the axon. The caliber, MT number, and MT density vary significantly from process to process, but on average are manyfold higher in the tau-induced processes than typically found in axons. Greater than 89% of the MTs in the processes are oriented with their plus ends distal to the cell body, and this proportion is even higher in the processes that are most similar to axons with regard to caliber, MT number, and MT density. Similar to the situation in the axon, MTs are discontinuous along the length of the tau-induced processes, and do not emanate from any observable nucleating structure in the cell body. We have also identified bundles of MTs throughout the cell bodies of the Sf9 cells induced to express tau. Similar to the MT arrays in the processes, these MT bundles are not visibly associated with any other cytological structures that might regulate their polarity orientation. Nevertheless, these bundles consist of MTs most (greater than 82%) of which have the same polarity orientation. Collectively, these results suggest that tau may play a fundamental role in generating MT organization in the axon. In particular, a key property of tau may be to bundle MTs preferentially with the same polarity orientation.     

Microtubule plus end‐tracking proteins play critical roles in directional growth of hyphae by regulating the dynamics of cytoplasmic microtubules in Aspergillus nidulans

Cytoplasmic microtubules (MTs) serve as a rate‐limiting factor for hyphal tip growth in the filamentous fungus Aspergillus nidulans. We hypothesized that this function depended on the MT plus end‐tracking proteins (+TIPs) including the EB1 family protein EBA that decorated the MT plus ends undergoing polymerization. The ebAΔ mutation reduced colony growth and the mutant hyphae appeared in an undulating pattern instead of exhibiting unidirectional growth in the control. These phenotypes were enhanced by a mutation in another +TIP gene clipA. EBA was required for plus end‐tracking of CLIPA, the Kinesin‐7 motor KipA, and the XMAP215 homologue AlpA. In addition, cytoplasmic dynein also depended on EBA to track on most polymerizing MT plus ends, but not for its conspicuous appearance at the MT ends near the hyphal apex. The loss of EBA reduced the number of cytoplasmic MTs and prolonged dwelling times for MTs after reaching the hyphal apex. Finally, we found that colonies were formed in the absence of EBA, CLIPA, and NUDA together, suggesting that they were dispensable for fundamental functions of MTs. This study provided a comprehensive delineation of the relationship among different +TIPs and their contributions to MT dynamics and unidirectional hyphal expansion in filamentous fungi.     

Dynamics of spindle fibers and microtubules during anaphase and phragmoplast formation

Detailed correlation of in vitro observations with the arrangement of microtubules (MTs) during anaphase-telophase were made on endosperm of Haemanthus katherinae. It is stressed that the general course of events leading to the formation of the phragmoplast is the same in all cells, but considerable variation of details may be found in different objects and even in various cells of the same tissue. The changes of MT arrangement in the interzonal region responsible for formation of the phragmoplast already occur in anaphase. During this stage continuous fibers (composed of numerous MTs) lengthen, become thinner (the number of MTs on a cross-section decreases), and often seem to break. After mid-anaphase, thin fibers begin to oscillate transversely to the axis of the phragmoplast and often are considerably laterally displaced (lateral movements). The longest MTs in the phragmoplast are present during oscillations and lateral movements. The new MTs arise in the phragmoplast regions depleted of MTs as a result of lateral movements (usually geometric central region of the phragmoplast). Clusters of vesicles, which accumulate in relation to MTs which move, fuse and form the cell plate. After the fusion, the number and the length of MTs decrease. Several processes are superimposed and occur simultaneously. Also the cell plate is, as a rule, in different stages of development in various regions of the phragmoplast. The movements of MTs and fusion of the vesicles is complex and the details of these processes are not entirely clear. The data supplied here modify some generally accepted concepts of phragmoplast formation and development. This concerns the center of origin of new MTs, the moment when they arise, and the way they subsequently behave.