Department of Physics, Graduate School of Science, The University of Tokyo, 7-3-1 Hongo Bunkyo-ku, Tokyo, 113-0033, Japan.
Center for Biosystems Dynamics Research, RIKEN, 6-2-3 Furuedai, Suita, Osaka, 565-0874, Japan.
Sci Rep. 2018 Nov 5;8(1):16333. doi: 10.1038/s41598-018-34549-7.
A power stroke of dynein is thought to be responsible for the stepping of dimeric dynein. However, the actual size of the displacement driven by a power stroke has not been directly measured. Here, the displacements of single-headed cytoplasmic dynein were measured by optical tweezers. The mean displacement of dynein interacting with microtubule was ~8 nm at 100 µM ATP, and decreased sigmoidally with a decrease in the ATP concentration. The ATP dependence of the mean displacement was explained by a model that some dynein molecules bind to microtubule in pre-stroke conformation and generate 8-nm displacement, while others bind in the post-stroke one and detach without producing a power stroke. Biochemical assays showed that the binding affinity of the post-stroke dynein to a microtubule was ~5 times higher than that of pre-stroke dynein, and the dissociation rate was ~4 times lower. Taking account of these rates, we conclude that the displacement driven by a power stroke is 8.3 nm. A working model of dimeric dynein driven by the 8-nm power stroke was proposed.
动力冲程的动蛋白被认为是二聚体动蛋白步进的原因。然而,动力冲程驱动的实际位移大小尚未直接测量。在这里,我们通过光学镊子测量了单个细胞质动蛋白的位移。在 100µM ATP 下,与微管相互作用的动蛋白的平均位移约为 8nm,并随着 ATP 浓度的降低呈 S 形下降。平均位移的 ATP 依赖性可以用一个模型来解释,即一些动蛋白分子在预冲程构象中与微管结合并产生 8nm 的位移,而其他动蛋白分子则在后冲程构象中结合并在不产生动力冲程的情况下脱离。生化分析表明,后冲程动蛋白与微管的结合亲和力比前冲程动蛋白高约 5 倍,解离速率低约 4 倍。考虑到这些速率,我们得出结论,动力冲程驱动的位移为 8.3nm。提出了一个由 8nm 动力冲程驱动的二聚体动蛋白的工作模型。