Hunt A J, Gittes F, Howard J
Department of Physiology and Biophysics, University of Washington, Seattle 98195.
Biophys J. 1994 Aug;67(2):766-81. doi: 10.1016/S0006-3495(94)80537-5.
Kinesin is a motor protein that uses the energy derived from the hydrolysis of ATP to power the transport of organelles along microtubules. To probe the mechanism of this chemical-to-mechanical energy transduction reaction, the movement of microtubules across glass surfaces coated with kinesin was perturbed by raising the viscosity of the buffer solution. When the viscosity of the solution used in the low density motility assay was increased approximately 100-fold through addition of polysaccharides and polypeptides, the longer microtubules, which experienced a larger drag force from the fluid, moved more slowly than the shorter ones. The speed of movement of a microtubule depended linearly on the drag force loading the motor. At the lowest kinesin density, where dilution experiments indicated that the movement was caused by a single kinesin molecule, extrapolation of the linear relationship yielded a maximum time-averaged drag force of 4.2 +/- 0.5 pN per motor (mean +/- experimental SE). The magnitude of the force argues against one type of "ratchet" model in which the motor is hypothesized to rectify the diffusion of the microtubule; at high viscosity, diffusion is too slow to account for the observed speeds. On the other hand, our data are consistent with models in which force is a consequence of strain developed in an elastic element within the motor; these models include a different "ratchet" model (of the type proposed by A. F. Huxley in 1957) as well as "power-stroke" models.
驱动蛋白是一种分子马达蛋白,它利用ATP水解产生的能量,沿着微管推动细胞器的运输。为了探究这种化学能到机械能转换反应的机制,通过提高缓冲溶液的粘度,干扰了微管在涂有驱动蛋白的玻璃表面上的移动。在低密度运动分析中使用的溶液,通过添加多糖和多肽使粘度增加了约100倍,较长的微管受到流体更大的阻力,移动速度比短微管慢。微管的移动速度与加载到马达上的阻力呈线性关系。在最低的驱动蛋白密度下,稀释实验表明移动是由单个驱动蛋白分子引起的,线性关系的外推得出每个马达的最大时间平均阻力为4.2±0.5皮牛(平均值±实验标准误差)。该力的大小与一种“棘轮”模型不符,在该模型中假设马达可纠正微管的扩散;在高粘度下,扩散太慢,无法解释观察到的速度。另一方面,我们的数据与力是马达内弹性元件产生应变的结果的模型一致;这些模型包括一种不同的“棘轮”模型(A.F.赫胥黎在1957年提出的那种类型)以及“动力冲程”模型。