The force generated by a detergent-extracted reactivated bull sperm flagellum during an isometric stall was measured with a force-calibrated glass microprobe. The average isometric stall force from 48 individual measurements was 2.5 +/- 0.7 x 10(-5) dyne (2.5 +/- 0.7 x 10(-10) N). The force measurements were obtained by positioning a calibrated microprobe in the beat path of sperm cells that were stuck by their heads to a glass microscope slide. The average position of the contact point of the flagellum with the probe was 15 microm from the head-tail junction. This average lever arm length multiplied by the measured force yields an estimate of the active bending moment (torque) of 3.9 x 10(-8) dyne x cm (3.9 x 10(-15) N x m). The force was sustained and was for the most part uniform, despite the fact that the flagellum beyond the point of contact with the probe usually continued beating. It appears that the dynein motors in the basal portion of the flagellum continue to pull in an isometric stall for as long as the motion of the flagellum is blocked. If dynein motors in the flagellum distal to the contact point with the probe were contributing force to the displacement of the probe, then the flagellar segment immediately past the point of contact would have to show a net curvature in the direction of the probe displacement. No such curvature bias was observed in the R-bend arrests, and only a small positive curvature bias was measured in the P-bend arrests. Our analysis of the data suggests that more than 90% of the sustained force component is generated by the part of the flagellum between the probe and the flagellar base. Based on this premise, the isometric stall force per dynein head is estimated to be 5.0 x 10(-7) dyne (5 pN). This equals approximately 1.0 x 10(-6) dyne (10 pN) per intact dynein arm. These values are close to the isometric stall force of isolated dynein. This suggests that all of the dynein heads between the base and the probe, on the active side of the axoneme, are contributing to the force exerted against the probe.
Cilia in many organisms undergo a phenomenon called ciliary reversal during which the cilia reverse the beat direction, and the cell swims backwards. Ciliary reversal is typically caused by a depolarizing stimulus that ultimately leads to a rise in intraciliary Ca++ levels. It is this increase in intraciliary Ca++ that triggers ciliary reversal. However, the mechanism by which an increase in intraciliary Ca++ causes ciliary reversal is not known. We have previously mutated the DYH6 gene of Tetrahymena thermophila by targeted gene knockout and shown that the knockout mutants (KO6 mutants) are missing inner arm dynein 1 (I1). In this study, we show that KO6 mutants do not swim backward in response to depolarizing stimuli. In addition to being unable to swim backwards, KO6 mutants swim forward at approximately one half the velocity of wild-type cells. However, the ciliary beat frequency in KO6 mutants is indistinguishable from that of wild-type cells, suggesting that the slow forward swimming of KO6 mutants is caused by an altered waveform rather than an altered beat frequency. Live KO6 cells are also able to increase and decrease their swim speeds in response to stimuli, suggesting that some aspects of their swim speed regulation mechanisms are intact. Detergent-permeabilized KO6 mutants fail to undergo Ca++-dependent ciliary reversals and do not show Ca++-dependent changes in swim speed after MgATP reactivation, indicating that the axonemal machinery required for these responses is insensitive to Ca++ in KO6 mutants. We conclude that Tetrahymena inner arm dynein 1 is not only an essential part of the Ca++-dependent ciliary reversal mechanism but it also may contribute to Ca++-dependent changes in swim speed and to the formation of normal waveform during forward swimming.
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