scholarly journals A Lateral Cap model of microtubule dynamic instability

FEBS Letters ◽  
1989 ◽  
Vol 259 (1) ◽  
pp. 181-184 ◽  
Author(s):  
Peter Bayley ◽  
Maria Schilstra ◽  
Stephen Martin
1997 ◽  
Vol 138 (1) ◽  
pp. 105-117 ◽  
Author(s):  
P.T. Tran ◽  
R.A. Walker ◽  
E.D. Salmon

The current two-state GTP cap model of microtubule dynamic instability proposes that a terminal crown of GTP-tubulin stabilizes the microtubule lattice and promotes elongation while loss of this GTP-tubulin cap converts the microtubule end to shortening. However, when this model was directly tested by using a UV microbeam to sever axoneme-nucleated microtubules and thereby remove the microtubule's GTP cap, severed plus ends rapidly shortened, but severed minus ends immediately resumed elongation (Walker, R.A., S. Inoué, and E.D. Salmon. 1989. J. Cell Biol. 108: 931–937). To determine if these previous results were dependent on the use of axonemes as seeds or were due to UV damage, or if they instead indicate an intermediate state in cap dynamics, we performed UV cutting of self-assembled microtubules and mechanical cutting of axoneme-nucleated microtubules. These independent methods yielded results consistent with the original work: a significant percentage of severed minus ends are stable after cutting. In additional experiments, we found that the stability of both severed plus and minus ends could be increased by increasing the free tubulin concentration, the solution GTP concentration, or by assembling microtubules with guanylyl-(α,β)-methylene-diphosphonate (GMPCPP). Our results show that stability of severed ends, particularly minus ends, is not an artifact, but instead reveals the existence of a metastable kinetic intermediate state between the elongation and shortening states of dynamic instability. The kinetic properties of this intermediate state differ between plus and minus ends. We propose a three-state conformational cap model of dynamic instability, which has three structural states and four transition rate constants, and which uses the asymmetry of the tubulin heterodimer to explain many of the differences in dynamic instability at plus and minus ends.


1991 ◽  
Vol 277 (3) ◽  
pp. 839-847 ◽  
Author(s):  
M J Schilstra ◽  
P M Bayley ◽  
S R Martin

The exchange of tubulin dimer into steady-state microtubules was studied over a range of solution conditions, in order to assess the effects of various common buffer components on the dynamic instability of microtubules. In comparison with standard buffer conditions (100 mM-Pipes buffer, pH 6.5, containing 0.1 mM-EGTA, 1.8 mM-MgC12 and 1 M-glycerol), the rate and extent of exchange, and thus of dynamic instability, are suppressed by increasing the concentration of glycerol above 2 M. Exchange is enhanced by the addition of further Mg2+ (up to 17 mM) or by the addition of Ca2+ (up to 0.4 mM). Phosphate ion (150 mM) has relatively little effect on the dynamic behaviour of microtubules, as judged by the exchange method. The findings are interpreted within the framework of the Lateral Cap model for microtubule dynamic instability, in terms of the effects of these changes on the intrinsic rate constants of the system. By contrast, the extent of tubulin exchange depends selectively on the value of the dissociation rate constant for tubulin-GDP. A decrease in the extent of exchange, and hence in dynamic activity, is associated with a decreased value for this rate constant, and vice versa. The results also show good agreement of predictions of the model in treating the observed variations in the dynamic properties of individual microtubules, induced by different solution conditions.


1989 ◽  
Vol 108 (3) ◽  
pp. 931-937 ◽  
Author(s):  
R A Walker ◽  
S Inoué ◽  
E D Salmon

The molecular basis of microtubule dynamic instability is controversial, but is thought to be related to a "GTP cap." A key prediction of the GTP cap model is that the proposed labile GDP-tubulin core will rapidly dissociate if the GTP-tubulin cap is lost. We have tested this prediction by using a UV microbeam to cut the ends from elongating microtubules. Phosphocellulose-purified tubulin was assembled onto the plus and minus ends of sea urchin flagellar axoneme fragments at 21-22 degrees C. The assembly dynamics of individual microtubules were recorded in real time using video microscopy. When the tip of an elongating plus end microtubule was cut off, the severed plus end microtubule always rapidly shortened back to the axoneme at the normal plus end rate. However, when the distal tip of an elongating minus end microtubule was cut off, no rapid shortening occurred. Instead, the severed minus end resumed elongation at the normal minus end rate. Our results show that some form of "stabilizing cap," possibly a GTP cap, governs the transition (catastrophe) from elongation to rapid shortening at the plus end. At the minus end, a simple GTP cap is not sufficient to explain the observed behavior unless UV induces immediate recapping of minus, but not plus, ends. Another possibility is that a second step, perhaps a structural transformation, is required in addition to GTP cap loss for rapid shortening to occur. This transformation would be favored at plus, but not minus ends, to account for the asymmetric behavior of the ends.


Author(s):  
R.A Walker ◽  
S. Inoue ◽  
E.D. Salmon

Microtubules polymerized in vitro from tubulin purified free of microtubule-associated proteins exhibit dynamic instability (1,2,3). Free microtubule ends exist in persistent phases of elongation or rapid shortening with infrequent, but, abrupt transitions between these phases. The abrupt transition from elongation to rapid shortening is termed catastrophe and the abrupt transition from rapid shortening to elongation is termed rescue. A microtubule is an asymmetrical structure. The plus end grows faster than the minus end. The frequency of catastrophe of the plus end is somewhat greater than the minus end, while the frequency of rescue of the plus end in much lower than for the minus end (4).The mechanism of catastrophe is controversial, but for both the plus and minus microtubule ends, catastrophe is thought to be dependent on GTP hydrolysis. Microtubule elongation occurs by the association of tubulin-GTP subunits to the growing end. Sometime after incorporation into an elongating microtubule end, the GTP is hydrolyzed to GDP, yielding a core of tubulin-GDP capped by tubulin-GTP (“GTP-cap”).


1988 ◽  
Vol 263 (21) ◽  
pp. 10344-10352
Author(s):  
M Caplow ◽  
J Shanks ◽  
R L Ruhlen

1994 ◽  
Vol 124 (3) ◽  
pp. 223-233 ◽  
Author(s):  
CL Rieder ◽  
ED Salmon

We argue that hypotheses for how chromosomes achieve a metaphase alignment, that are based solely on a tug-of-war between poleward pulling forces produced along the length of opposing kinetochore fibers, are no longer tenable for vertebrates. Instead, kinetochores move themselves and their attached chromosomes, poleward and away from the pole, on the ends of relatively stationary but shortening/elongating kinetochore fiber microtubules. Kinetochores are also "smart" in that they switch between persistent constant-velocity phases of poleward and away from the pole motion, both autonomously and in response to information within the spindle. Several molecular mechanisms may contribute to this directional instability including kinetochore-associated microtubule motors and kinetochore microtubule dynamic instability. The control of kinetochore directional instability, to allow for congression and anaphase, is likely mediated by a vectorial mechanism whose magnitude and orientation depend on the density and orientation or growth of polar microtubules. Polar microtubule arrays have been shown to resist chromosome poleward motion and to push chromosomes away from the pole. These "polar ejection forces" appear to play a key role in regulating kinetochore directional instability, and hence, positions achieved by chromosomes on the spindle.


2017 ◽  
Vol 31 (S1) ◽  
Author(s):  
Zachary R Gergely ◽  
Patrick J Flynn ◽  
Salvador Montes ◽  
J. Richard McIntosh ◽  
M. D. Betterton

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