Qian H, Elson E L, Frieden C
Department of Biochemistry and Molecular Biophysics, Washington University School of Medicine, St. Louis, Missouri 63110.
Biophys J. 1992 Oct;63(4):1000-10. doi: 10.1016/S0006-3495(92)81686-7.
Fluorescence correlation spectroscopy (FCS) has been used to measure the diffusion of fluorescently labeled beads in solutions of polymerized actin or buffer. The results, obtained at actin concentrations of 1 mg/ml, show that small beads (0.09 micron in diameter) diffuse nearly as rapidly in the actin gel as in buffer, whereas the largest beads tested (0.5 micron in diameter) are immobilized. Measured autocorrelation times for motions of beads with intermediate sizes show that the diffusion is retarded (relative to buffer) and that the time behavior cannot be represented as a single diffusive process. In addition to the retarded diffusion observed over distances > 1 micron, 0.23-micron beads also show a faster motion over smaller distances. Based on the measured rate of this faster motion, we estimate that the beads may be constrained within a cage approximately 0.67 micron on a side, equal to a filament length of approximately 250 subunits. Fluorescence correlation spectroscopy measurements made in the same small spot (radius of 1.4 microns) of the gel vary over time. From the variations of both the autocorrelation functions and the mean fluorescence, we conclude that, corresponding to a spatial scale of 1.4 microns, the actin gel is a dynamic structure with slow rearrangement of the gel occurring over periods of 20-50 s at 21-22 degrees C. This rearrangement may result from local reorganization of the actin matrix. Data for the retardation of beads by the actin gel are consistent with a detailed theory of the diffusion of particles through solutions of rigid rods that have longitudinal diffusion coefficients much less than that of the particles (Ogston, A. G., B. N. Preston, and J. D. Wells. 1973. Proc. R. Soc. Lond. A. 333:297-316).
荧光相关光谱法(FCS)已被用于测量荧光标记的珠子在聚合肌动蛋白溶液或缓冲液中的扩散。在肌动蛋白浓度为1mg/ml时获得的结果表明,小珠子(直径0.09微米)在肌动蛋白凝胶中的扩散速度几乎与在缓冲液中一样快,而测试的最大珠子(直径0.5微米)则被固定。对中等尺寸珠子运动的测量自相关时间表明,扩散受到阻碍(相对于缓冲液),并且时间行为不能表示为单个扩散过程。除了在距离>1微米时观察到的扩散受阻外,0.23微米的珠子在较小距离上也显示出更快的运动。根据这种更快运动的测量速率,我们估计珠子可能被限制在边长约0.67微米的笼子内,相当于约250个亚基的细丝长度。在凝胶的同一个小斑点(半径1.4微米)中进行的荧光相关光谱测量随时间变化。从自相关函数和平均荧光的变化中,我们得出结论,对应于1.4微米的空间尺度,肌动蛋白凝胶是一种动态结构,在21-22摄氏度下,凝胶的缓慢重排在20-50秒的时间段内发生。这种重排可能是由于肌动蛋白基质的局部重组。肌动蛋白凝胶对珠子的阻碍数据与颗粒通过纵向扩散系数远小于颗粒的刚性棒溶液扩散的详细理论一致(奥格斯顿,A.G.,B.N.普雷斯顿,和J.D.威尔斯。1973.《英国皇家学会学报》A.333:297-316)。