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Vol. 17, Issue 3, 1451-1460, March 2006
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Cell Biology and Biophysics Program, European Molecular Biology Laboratory, 69117 Heidelberg, Germany
Submitted April 1, 2005;
Revised December 5, 2005;
Accepted January 3, 2006
Monitoring Editor: Erika Holzbaur
| ABSTRACT |
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| INTRODUCTION |
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Depletion experiments in Xenopus egg extracts have shown that Xkid is essential for metaphase chromosome alignment but is not required for bipolar spindle assembly (Antonio et al., 2000
; Funabiki and Murray, 2000
). Xkid seems to be a typical transporter, powering chromosome arms in an antipoleward manner, therefore contributing to the so-called polar wind involved in chromosome alignment (Carpenter, 1991
; Heald, 2000
). Although Xklp1 was also originally proposed to participate in chromosome alignment, different experimental strategies have lead to the idea that its main function is in spindle formation and maybe cytokinesis (Vernos et al., 1995
). Depletion of Xklp1 by antisense oligonucleotide injection in Xenopus oocytes resulted in the strong inhibition of early embryonic cell divisions with incomplete furrow ingression and aberrant mitotic figures (Vernos et al., 1995
). This approach showed that Xklp1 is essential for the early embryonic cell divisions. Subsequently, a more specific role for Xklp1 in spindle assembly was proposed, based on the spindle phenotypes observed upon addition of anti-Xklp1 antibody to Xenopus egg extracts: sperm nuclei formed unstable bipolar spindles with reduced microtubule density and chromosome alignment defects (Vernos et al., 1995
), and DNA-coated beads formed either compact microtubule bundles or detached from organized half-spindles (Walczak et al., 1998
). These phenotypes suggested that Xklp1 participates in spindle pole extension and mediates chromosome-microtubule interactions. We have now reexamined the role of Xklp1 by monitoring spindle assembly and microtubule behavior in Xenopus egg extracts containing different concentrations of this chromokinesin.
| MATERIALS AND METHODS |
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Expression and Purification of Full-length Xklp1
The full-length Xklp1 cDNA (Vernos et al., 1995
) was inserted into the plasmid pFastBac and sequenced to confirm the absence of mutations. Recombinant virus was produced with the Bac-to-Bac Baculovirus expression system (Life Technology). For expression, 50 ml of Sf9 cells (2 x 106 cells/ml) were infected for 48 h. For purification, cells were washed in ice-cold PBS and resuspended in 2.5 ml of lysis buffer I (50 mM Na-phosphate, 10 mM KCl, 5 mM
-mercaptoethanol, and protease inhibitors; Complete EDTA-free, Roche). The suspension was homogenized with 25 strokes in a B-type douncer and centrifuged in a JA2550 Beckman rotor at 27,000 rcf (
15,000 rpm) for 10 min at 4°C. The resulting pellet was reextracted with 1 ml of lysis buffer II (50 mM Na-phosphate, 900 mM KCl, 5 mM MgCl2, 10% glycerol, 0.1% Tween20, 5 mM
-mercaptoethanol, and protease inhibitors; Complete EDTA-free, Roche) for 30 min on ice. The suspension was homogenized with 25 strokes in a B-type douncer and centrifuged in a JA2550 Beckman rotor at 27,000 rcf (
15,000 rpm) for 10 min at 4°C. The two supernatants were combined and mixed in batch with 1 ml of Talon resin (Clontech, Palo Alto, CA) equilibrated with washing buffer (50 mM Na-phosphate, 250 mM KCl, 10% glycerol, 2.5 mM
-mercaptoethanol, and protease inhibitors; Complete EDTA-free, Roche) and mixed at 4°C for 60 min The resin was extensively washed with washing buffer containing 15 mM imidazole and loaded on a column. The recombinant protein was eluted with 8 x 0.5 ml of washing buffer containing 200 mM imidazole.
Spindle Assembly and Aster Experiments
Spindle assembly was induced in Xenopus egg extract as previously described (Sawin and Mitchison, 1991
). Centrosomal asters were assembled by addition of purified human centrosomes (Bornens and Moudjou, 1999
) to CSF extracts containing rhodamine or Cy3-labeled tubulin. For add-back experiments, recombinant full-length Xklp1 (1- to 3-fold endogenous concentration) or the equivalent volume of buffer was added to mock- or Xklp1-depleted extracts when the extract was cycled back into M-phase. For centrosome aster formation in the presence of increasing concentrations of Xklp1, purified centrosomes were incubated with different concentrations of Xklp1 or buffer for 5 min on ice before addition to the CSF extract. For immunofluorescence analysis asters or spindles were diluted with 1 ml of dilution buffer (BRB80, 15% glutaraldehyde, 0.5% glycerol, 1% Triton X-100 for asters, and BRB80, 30% glycerol, 1% Triton X-100 for spindles) and pelleted on coverslips at 22,500 rcf for 12 min at 20°C through a 5 ml glycerol cushion (BRB80, 25% glycerol for asters, 40% glycerol for spindles). Coverslips were fixed for 10 min in cold methanol (20°C), quenched for 10 min in PBS containing 0.1% sodium borohydrate (Sigma, St. Louis, MO) and processed for immunofluorescence.
Antibodies and Western Blot
Ab03 is a polyclonal antibody raised against a fragment of the stalk domain of Xklp1 (Walczak et al., 1998
). P2E9 is a monoclonal antibody (mAb) raised against the tail domain of Xklp1 (Vernos et al., 1995
). Tubulin was detected with the mAb DM1 (Sigma) or with in-house-produced polyclonal antitubulin antibodies. For immunoblotting, equivalent amounts of treated and untreated egg extracts were resolved on an 8% SDS-gel and transferred onto a nitrocellulose membrane. Membranes were incubated with Ab03 or P2E9 and with a secondary IgG-HRP-conjugate (Dianova). Blots were developed using an ECL (Amersham, Indianapolis, IN) chemiluminescence detection system.
Microtubule Pelleting Assay
Microtubule pelleting assays were carried out as described (Budde et al., 2001
). In brief, centrosomal asters or bipolar spindles were diluted in 500 µl of dilution buffer in the absence of glutaraldehyde and layered onto 500 µl of cushion buffer (see above) in a 1.5-ml Eppendorf tube. Samples were centrifuged at 10,000 rpm (
12,000 rcf) for 10 min at room temperature. Supernatants were delicately aspirated, and the interface between supernatant and cushion was rinsed with dilution buffer. Microtubule pellets were dissolved in 30 µl of SDS sample buffer and resolved in 8% SDS-PAGE. Tubulin and Xklp1 contents were analyzed by immunoblot. In add-back experiments, recombinant full-length Xklp1 (at endogenous concentration) or an equivalent volume of buffer was added to mock- or Xklp1-depleted extracts as the extract was cycled back into M-phase. To induce microtubule depolymerization, nocodazole (Sigma) was added to the extracts after cycling the extracts back to mitosis.
Microtubule Dynamics Assay and Data Analysis
Analysis of microtubule dynamics was carried out as described (Tournebize et al., 1997
). Ten microliters of frozen CSF-extract, 0.5 µl of Cy3-labeled tubulin (10 mg/ml), 0.3 µl of human centrosomes (1 x 105 centrosomes/µl), and 0.5 µl of saturated hemoglobin solution (in CFS-XB) were mixed on ice. This mix, 1.8 µl, was then squashed under an 18 x 18-mm coverslip and placed under the fluorescence microscope (all glasses were cleaned with ethanol and rinsed in water). Microtubules were imaged using a Zeiss Axiovert 135 microscope (Thornwood, NY) equipped with a x100 oil-immersion objective and a long-pass rhodamine filter. Images were captured with a CoolSnap CCD (charged-coupled device) camera controlled by Methamorph software (Universal Imaging, West Chester, PA). In a typical experiment, images were taken every 2 s for 5 min. The four parameters defining microtubule dynamics were determined as follows: microtubule growth (or shrinkage) had to persist for at least six consecutive frames (10 s), with a net change in length of at least 0.5 µm. Catastrophe and rescue frequencies were determined by dividing the number of catastrophe or rescue events by the total time microtubules spent growing or shrinking.
The microtubule steady state length
L
was calculated as described in (Verde et al., 1992
) using the equation:
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Immunofluorescence and Quantifications
For indirect immunofluorescence, coverslips were fixed for 10 min in cold (20°C) methanol. Fixed samples were then either immediately processed for immunostaining or stored until use at 4°C in PBS. Coverslips were rehydrated for 10 min in PBS-T and incubated first with the primary antibody in PBS-T and then with the secondary antibody (Alexa Fluor-568 or -488 [Molecular Probes] labeled anti-mouse and anti-rabbit antibodies) in PBS-T, both for 20 min at room temperature. DNA was stained with 5 µg/ml Hoechst dye in PBS-T. For quantifications, nonsaturated images of randomly selected spindles and asters were taken using the same camera settings. The total microtubule fluorescence associated with each spindle and aster was then measured using ImageJ (NIH). Measurement of spindle length and width was carried out using Analysis (Soft Imaging System) and ImageJ software. For analysis of total DNA and tubulin content associated with each spindle, confocal slices of constant thickness were taken throughout the spindles on an LSM-510 confocal microscope (Zeiss) equipped with a x63 oil-immersion objective. The intensities of microtubules or DNA fluorescence were measured on each slice with ImageJ. The total intensities were calculated by addition of the single slice values. Determination of aster average length and average tubulin content was carried out using a custom-made macro running on Matlab software (MathWorks, Natick, MA), as described in Gruss et al. (2002
). To discriminate between spindle shapes, we calculated the average width of all spindles assembled in the control extract and defined as barrel-like all spindles wider than the average width + 1 SD. The data were subjected to statistical analysis using an unpaired Student's t test (http://www.physics.csbsju.edu/stats/ttest.html).
| RESULTS |
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We first performed CSF spindle assembly reactions using mock- and Xklp1-depleted extracts. Incubation of sperm nuclei in CSF-extract for 45 min resulted in the formation of monopolar half-spindles and bipolar spindles in mock-depleted extracts (Figure 1B). Similar structures were also observed in Xklp1-depleted extracts, but the proportion of bipolar spindles was reduced compared with the control (18% in Xklp1-depleted extract vs. 27% in mock-depleted extract; Figure 1C). Moreover, we observed that in a majority of the half-spindles assembled in Xklp1-depleted extract, chromatin positioning was incorrect. In these half-spindles, the chromosomes were often immersed in the microtubule array instead of stretching at microtubule-splayed plus-ends as in the control (Figure 1B). Therefore, in accordance with previous experiments, we found that in CSF spindle assembly reactions, Xklp1 depletion affects bipolar spindle formation and chromosome positioning.
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Altogether these data suggested that Xklp1 plays a role in positioning chromatin at microtubule plus-ends and in efficient bipolar spindle formation.
Spindles Assembled in Xklp1-depleted Extracts Have an Increased Microtubule Mass
Although quantifying bipolar spindles formed in cycled extracts, we noticed that in the absence of Xklp1 several spindles did not show the typical fusiform shape but appeared to be wider, adopting a barrel-like morphology (Figure 3A). To quantify this phenotype, we arbitrarily classified as barrel-like all spindles whose width was larger than the average width + 1 SD. Results from three independent experiments showed that nearly half of the bipolar spindles assembled in Xklp1-depleted extracts had a barrel-like shape, whereas only 16% showed a similar morphology in mock-depleted extracts (Figure 3B). To try to understand what was causing this phenotype, we first quantified the total amount of polymerized tubulin associated with individual spindles formed in the presence or absence of Xklp1. As shown in Figure 3C, the distribution of tubulin fluorescence intensities of spindles formed in Xklp1-depleted extract was shifted to higher values than that of spindles assembled in mock-depleted extracts. This indicated that an increase in microtubule mass could be at the origin of the barrel-like spindle phenotype. To determine whether this increase was due to changes in microtubule length and/or number, we measured the length and width of bipolar spindles assembled in the different extracts. We found a similar distribution of spindle lengths for the two types of extracts. However, the distribution of widths of spindles assembled in Xklp1-depleted extract was shifted toward higher values than that of spindles assembled in mock-depleted extracts (Figure 3D). These results (total tubulin fluorescence intensity, spindle length and width) were always consistent in three independent experiments. Finally, to rule out that the increase in microtubule mass of spindles assembled in Xklp1-depleted extract could be related to a higher content of chromatin due, for example, to the clustering of several sperm nuclei, we quantified the fluorescence intensities of both tubulin and DNA in individual spindles formed in the different extracts (Figure 3E). Most spindles assembled in mock- and Xklp1-depleted extracts had similar DNA fluorescence intensity values, although a few contained more chromatin, probably due to sperm nuclei clustering (top part of Figure 3D). However, for similar DNA fluorescence levels, the tubulin fluorescence intensity of spindles assembled in Xklp1-depleted extracts was on average 50% higher than those assembled in mock-depleted extracts (Figure 3E, Table 1). This analysis confirmed that spindles assembled in Xklp1-depleted extracts had a higher microtubule content than those assembled in control extracts.
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To rule out that other important protein(s) could be codepleted with Xklp1 during immunoprecipitation, we checked whether adding purified recombinant Xklp1 to Xklp1-depleted extracts could fully rescue the depletion phenotype. We estimated Xklp1 endogenous concentrations to be in the range of 0.40.9 µM in CSF-arrested egg extracts (unpublished data) and added recombinant full-length Xklp1 in the depleted egg extract to restore Xklp1 physiological concentration (Figure 4A). Immunofluorescence analysis showed that the recombinant protein localized to the chromosomes like endogenous Xklp1 (Figure 4B) and that it was able to rescue both the efficiency of bipolar spindle assembly (Figure 4C, top panel) and the fusiform shape of the spindles (Figure 4C, bottom panel).
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As a complementary approach to verify that Xklp1 affects microtubule polymerization, spindles assembled in mock- and Xklp1-depleted extracts, supplemented or not with recombinant full-length protein, were pelleted through a glycerol cushion, and the resulting pellets were analyzed by Western blotting. We observed consistently an increase in tubulin in the microtubule pellets obtained from spindles assembled in Xklp1-depleted extracts compared with those assembled in control extracts or in Xklp1-depleted extract containing recombinant protein (Figure 4A). These results again indicated strongly that Xklp1 exerts a negative effect on microtubule polymerization in the M-phase extract.
Altogether the different analysis performed in Xklp1-depleted egg extracts suggested that Xklp1 somehow limits the total mass of microtubules engaged in bipolar spindle formation. In its absence, the efficiency of bipolar spindle formation decreases and spindles have an altered shape that is most probably related to an increase in microtubule number since microtubule length seems unaffected.
Increasing Xklp1 Concentration in the Egg Extract Results in the Reduction of the Spindle Microtubule Mass
We reasoned that if Xklp1 activity limits somehow microtubule polymerization during spindle assembly, increasing its concentration in the egg extract should result in the opposite effect. We therefore increased the concentration of Xklp1 by a factor of 23 in the egg extract and examined cycled spindle formation under these conditions (Figure 5A). We found that bipolar spindles formed as efficiently in the presence of high Xklp1 concentrations as in control extract (unpublished data). However, the quantitative analysis of the tubulin fluorescence intensity of spindles revealed that those assembled in extracts containing more Xklp1 had a lower tubulin content than those assembled in control extracts (Figure 5, B and C). These results were consistent with the previous ones and supported the view that Xklp1 has a negative effect on microtubule polymerization during M-phase.
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These results encouraged us to use the aster assay to investigate further the role of Xklp1 in microtubule assembly.
Xklp1 Reduces Microtubule Polymerization from Centrosomes
Purified centrosomes were incubated in mock- and Xklp1-depleted extracts, fixed, and pelleted onto coverslips (Figure 7). The total tubulin fluorescence intensity associated with individual asters was then measured and the asters were classified into empirically defined categories of fluorescence intensity (Figure 7B). Most asters assembled in mock-depleted extracts (52%) had low tubulin fluorescence intensity values and only 14% belonged to the highest tubulin fluorescence intensity category. By contrast, asters assembled in Xklp1-depleted extracts showed an inverse distribution: the largest number had high tubulin fluorescence intensity values (51%), whereas only 18% corresponded to the lowest tubulin fluorescence intensity category.
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The increase in tubulin content of asters formed in Xklp1-depleted extract could be due to an increase in microtubule length and/or to an increase in the number of microtubules per aster. To investigate this issue, we determined the average length of microtubules in asters formed in the different extracts. We found a mild increase for this value in asters assembled in Xklp1-depleted extracts versus mock-depleted extracts (Table 2). Interestingly, there was a direct correlation between the concentration of Xklp1 in the extract and the average length of microtubules in asters (
Xklp1 >
Xklp1 + 0.8 µM > Mock >
Xklp1 + 1.6 µM). Addition of recombinant Xklp1 to the depleted extract rescued microtubule length. However, the small change in microtubule length could not account for the average 10-fold difference in total tubulin fluorescence intensity between asters assembled in mock- and Xklp1-depleted extracts. These results suggested that asters formed in Xklp1-depleted extracts have more microtubules than those assembled in mock-depleted extracts.
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Xklp1 Depletion Has a Mild Influence on Microtubule Rescue and Catastrophe Frequencies
One possible way by which Xklp1 could influence microtubule polymerization is by changing the parameters defining microtubule dynamic instability. We therefore followed individual microtubules nucleated by centrosomes in mock- and Xklp1-depleted M-phase extracts by time-lapse fluorescence microscopy and determined the four parameters defining microtubule dynamic instability in the presence and absence of Xklp1 (Table 3). The velocities of microtubule growth and shrinkage did not change significantly in the presence or absence of Xklp1. However, there was a mild effect on the frequencies of rescues and catastrophes. In Xklp1-depleted extracts: microtubules rescue frequency increased by 62% (1.17 vs. 0.72 events/min) and the catastrophe frequency increased by 20% (2.49 vs. 2.08 events/min; Table 3). The slightly stronger effect on the rescue frequency suggested that microtubules could be longer in Xklp1-depleted extract. Using the measured parameters, we calculated a steady-state microtubule length of 5.092 µm for asters assembled in mock-depleted extracts and 5.598 µm for asters assembled in Xklp1-depleted extracts (Verde et al., 1992
). This could explain the increase average size of microtubules measured experimentally for asters assembled in Xklp1-depleted extracts versus mock-depleted extracts. However, this could not account for the increase in microtubule mass observed in spindles and asters assembled in Xklp1-depleted extracts. Again this suggested that the primary effect of Xklp1 depletion is an increase in microtubule number.
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Xklp1 Affects the Early Stages of Centrosomal Microtubule Elongation
We then tried to find an experimental setting that would enable us to examine a potential effect of Xklp1 on the early steps of microtubule nucleation versus a more general effect on microtubule assembly. M-phase extracts were supplemented with buffer, 0.5 or 1 µM recombinant Xklp1, and purified centrosomes. Samples were taken after 1 min to examine the phases of microtubule nucleation and early elongation and after 10 min to examine asters at steady state (Figure 8). At 1 min, asters assembled in the presence of the higher amount of recombinant Xklp1 (1 µM) had a reduced microtubule mass compared with the other conditions (Figure 8A, top panel, and Table 4). This effect was much stronger after 10 min of incubation and was also obvious in samples containing lower concentrations of recombinant Xklp1 (Figure 8A, bottom panel, and Table 4). These data indicated that Xklp1 influences microtubule aster formation from very early on when microtubule nucleation and/or early elongation is the limiting factor. It suggests that Xklp1 has some role in limiting the efficiency of microtubule elongation off the centrosome leading to a decrease in microtubule number and therefore in total microtubule mass.
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| DISCUSSION |
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The Role of Xklp1 in Pole Extension and Chromosome Positioning
The phenotypes observed previously in egg extracts containing anti-Xklp1 antibodies upon addition of sperm nuclei and chromatin beads suggested that Xklp1 takes part in spindle pole extension and chromosome alignment (Vernos et al., 1995
; Walczak et al., 1998
). We show here that depletion of Xklp1 from Xenopus egg extracts does not completely impair spindle formation. However, in the absence of Xklp1 bipolar spindles need more time to assemble and, at any given time, the percentage of fully formed bipolar spindles is lower than in control extracts. This suggests that although Xklp1 is not a major player in establishing spindle bipolarity, it contributes to its efficiency.
We did not observe major defects in chromosome alignment in spindles formed in Xklp1-depleted cycled extracts. This suggests that the relatively strong chromosome misalignment defects observed previously upon anti-Xklp1 antibody addition to the extract may not have been solely due to the direct inhibition of Xklp1 but could have arisen through some indirect effect due to the presence of the antibody on the surface of the chromosome (Vernos et al., 1995
). However, we have now observed that chromosomes are mispositioned in the majority of half-spindles formed in Xklp1-depleted noncycled extracts. This suggests that the balance of forces involved in positioning chromosomes may differ between cycled and noncycled extracts. In fact, sperm chromosomes incubated in CSF extract do not replicate before inducing half-spindle formation. Therefore, in noncycled extracts kinetochores are not paired and may be functionally immature and unable to establish a bipolar attachment. As a result it is possible that in these conditions, chromosomes are more sensitive to the imbalance of forces as suggested by the mispositioning of chromosomes in the absence of Xklp1. Altogether, these data indicate that Xklp1 has indeed some role in moving or maintaining chromosome arms at microtubule plus-ends. Recent studies in vitro have indeed shown that Xklp1 is a plus-end directed motor (Bringmann et al., 2004
), and it is thus possible that it participates in the generation of forces moving chromosome arms in an antipoleward manner and/or in pole extension as previously proposed. However, our results indicate that Xklp1 does not provide the major forces involved in chromosome positioning in egg extract. Most of these forces are most likely powered by another Xenopus chromokinesin, Xkid (Antonio et al., 2000
; Funabiki and Murray, 2000
).
Control of Spindle Microtubule Polymer Mass by Xklp1
Centrosomal asters and spindles assembled in cycled extracts containing different concentrations of Xklp1 yield consistent phenotypes, suggesting that Xklp1 regulates negatively microtubule density in M-phase extracts. Changes in the parameters defining microtubule dynamics have a direct influence on the length and mass of polymerized tubulin at steady state. In M-phase, microtubules become short and highly unstable. This is due to a several fold increase in microtubule catastrophe frequency as the systems change from interphase to M-phase (Verde et al., 1992
; Karsenti and Vernos, 2001
). The major catastrophe factor in the M-phase Xenopus egg extract is XKCM1, a Kinesin-13 family member. XKCM1 depletion results in a major increase of microtubule length and this impairs spindle formation in egg extract (Walczak et al., 1996
). Xklp1 depletion results in a much milder phenotype. Microtubules are slightly longer but the increase in total microtubule polymer in centrosomal asters and spindles is proportionally much higher, suggesting that the major effect is an increase of microtubule number.
We considered the possibility of a direct negative influence of Xklp1 on the rate of microtubule nucleation in M-phase and tested this idea by comparing the number of microtubule asters induced by RanGTP in mock-depleted and Xklp1-depleted extracts. In our experimental setting we did not see a difference in the ability of RanGTP to induce microtubule aster formation in M-phase egg extract in the absence or presence of Xklp1 (unpublished data). However, we observed a small decrease in total tubulin mass in the early phases of centrosome-directed aster formation in egg extract containing an excess of Xklp1. Because Xklp1 does not localize to the centrosome it is unlikely that it has a role in modulating microtubule nucleation per se. However, our data suggest that it limits microtubule early elongation off the centrosome. The parameters for dynamic instability in Xklp1-depleted extract suggest that microtubules are slightly more dynamic when Xklp1 is absent. Because the rescue frequency increases proportionally more (62%) than the catastrophe frequency (20%), this could explain why at steady state there are more microtubules under conditions of high microtubule nucleation frequency as is the case around mitotic chromosomes or centrosomes.
Recent studies on the kinetic properties of Xklp1 motor domain have shown that it strongly influences microtubule dynamics, slowing down both microtubule growth and shrinkage in asters formed in pure tubulin solution (Bringmann et al., 2004
). Motor, at 10 µM, was required to block microtubule growth completely (in the presence of a large excess of tubulin), whereas 1 µM was sufficient to inhibit microtubule depolymerization completely (in the absence of free tubulin). In the extract, we estimated a concentration for Xklp1 of
0.40.9 µM in solution. This is in the lower range of the effective concentration producing a clear effect in vitro. Although we do not know the concentration of Xklp1 on the chromosome arms, it seems to be highly enriched there and therefore the in vitro results suggested that its depletion could result in more dramatic spindle phenotypes. However, there might be several reasons to account for this in addition to the concentration factor: 1) some of the properties of the full-length protein may differ from those of the motor domain alone, and 2) several other factors are involved in the regulation of microtubule dynamics in the M-phase egg extract and it is difficult to predict how Xklp1 may cooperate or compete with them for microtubule binding.
Nevertheless, the effect of Xklp1 depletion on microtubule catastrophe and rescue frequencies in the egg extract is in accordance with the measurements made with Xklp1 motor domain in vitro. The decrease of microtubule rescue and catastrophe frequencies by Xklp1 in the extract certainly results in a reduction of microtubule dynamics. Altogether, this could contribute to the stabilization of microtubules around chromosomes, as was previously suggested (Vernos et al., 1995
; Walczak et al., 1996
) and at the same time it may decrease the overall microtubule number. In this context, the barrel-like shape of spindles assembled in the absence of Xklp1 could arise both from an increase in microtubule number and from the inefficient movement of microtubules toward the spindle poles. Recent studies aimed at understanding the mechanisms that govern spindle length in the Xenopus egg extract system have lead the authors to propose the existence of a hypothetical tensile element or matrix attached to the poles and extending toward the spindle equator (Mitchison et al., 2005
). Another nonexclusive possibility is that this tensile element may force the spindle to adopt a barrel-like morphology when the forces provided by the chromokinesin are absent and/or the number of microtubules present is larger.
Although we can visualize the mitotic spindle as a finite entity, it is in fact an extremely dynamic assembly of molecules (Karsenti and Vernos, 2001
; Wittmann et al., 2001
). Several key features are integrated into this self-organizing process: microtubule length, microtubule organization, and spindle volume. Here we have shown that the Xenopus kinesinlike protein Xklp1 participates in this process by exerting a control on the number of microtubules in the spindle. Preliminary experiments indicate that this may be an important function because spindles formed in Xklp1-depleted extract do not seem to be fully competent for chromosome segregation (unpublished data). Further experiments will be needed to determine how important this mechanism is for spindle functionality.
| ACKNOWLEDGMENTS |
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| Footnotes |
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Address correspondence to: Isabelle Vernos (isabelle.vernos{at}crg.es).
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