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The propagation of a zone of activation along groups of flagellar doublet microtubules.

作者信息

Vernon G G, Woolley D M

机构信息

Department of Physiology, University of Bristol, United Kingdom.

出版信息

Exp Cell Res. 1995 Oct;220(2):482-94. doi: 10.1006/excr.1995.1340.

Abstract

The complexity of the 9 + 2 flagellar axoneme has made it difficult to discover the mechanism of bend propagation. We have studied a simplified preparation of mechanically "opened-out" groups of doublet microtubules that adopt a helical, ribbon-like form. From the very long sperm of the quail, ribbons of doublets up to 130 microns long have been obtained. We reactivated them photolytically by releasing ATP from caged ATP, thus observing the reactivation from the beginning. The response to ATP was a reduction in the pitch and diameter of the helix, in what we refer to as an "active zone" (AZ). Ahead of the AZ was a short region of increase in helical pitch and diameter, the pre-AZ. We ascribe these two altered geometries to the development of tension between the doublets, actively (in the AZ) and passively (in the pre-AZ). The AZ/pre-AZ complex established itself at one end of a helix--almost certainly the proximal end--then it propagated toward the other end of the helix at a mean velocity of 15 microns s-1 (using 1 mM caged ATP), maintaining or increasing its length as it traveled. This is the same velocity as that for bend propagation on cylindrical axonemes detached from their basal structures. Successive propagations on the same helix were seen. Thus, active and inactive segments of the same doublet assembly can coexist, even though all parts are exposed to ATP. The motor response is seen to be a localized event that is transmitted metachronally. The propagation of activation is an intrinsic property of structures in the interdoublet gap and does not require constituents of the cytosol other than ATP and Mg2+. Since it occurs in helical ribbons (3 + 0, 4 + 0, etc.), the propagation of activity must be independent of central axonemal structures; furthermore, it cannot be dependent on the integrity of the 9 + 2 cylinder nor on any feedback from large-scale features of the waveform.

摘要

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