Haskell R C, Carlson F D
Biophys J. 1981 Jan;33(1):39-62. doi: 10.1016/S0006-3495(81)84871-0.
Measurements were made of the intensity autocorrelation function, g(2)[tau], of light scattered from intact frog muscle fibers. During the tension plateau of an isometric tenanus, scattered field statistics were approximately Gaussian and intensity fluctuations were quasi-stationary. The half time, tau 1/2, for the decay of g(2)[tau] was typically 70 ms at a scattering angle of 30 degrees. The decay rate, 1/tau 1/2, of g(2)[tau] varied roughly linearly with the projection of the scattering vector on the fiber axis. 1/tau 1/2 was greater during the tension creep phase of tetani of highly stretched fibers, but was roughly independent of sarcomere length during the tension plateau. g(2)[tau] measured during rest or on diffraction pattern maxima during isometric contraction were flat with low amplitudes. These results are consistent with a model of a 200-mu m segment of an isometrically contracting fiber in which scattering material possesses relative axial velocities of 1-2 mu m/s accompanied by relative axial displacements greater than 0.1 mu m. The slow (1-2 mu m/s) motion of one portion of the fiber relative to another observed under the microscope (500X) during isometric contraction is consistent with the light-scattering results. Structural fluctuations on the scale of the myofibrillar sarcomere which may arise from asynchronous cycling of cross-bridges must involve relative axial velocities less than 3 mu m/s or relative axial displacements less than 0.05 mu m.
对完整青蛙肌肉纤维散射光的强度自相关函数(g^{(2)}(\tau))进行了测量。在等长强直收缩的张力平台期,散射场统计量近似为高斯分布,强度涨落为准静态的。在散射角为30度时,(g^{(2)}(\tau))衰减的半值时间(\tau_{1/2})通常为70毫秒。(g^{(2)}(\tau))的衰减率(1/\tau_{1/2})大致与散射矢量在纤维轴上的投影呈线性变化。在高度拉伸纤维的强直收缩的张力蠕变阶段,(1/\tau_{1/2})更大,但在张力平台期大致与肌节长度无关。在静息时或等长收缩期间衍射图样最大值处测量的(g^{(2)}(\tau))是平坦的,幅度较低。这些结果与等长收缩纤维的200微米段模型一致,在该模型中,散射物质具有1 - 2微米/秒的相对轴向速度,并伴有大于0.1微米的相对轴向位移。在等长收缩期间在显微镜(500倍)下观察到的纤维一部分相对于另一部分的缓慢(1 - 2微米/秒)运动与光散射结果一致。肌原纤维肌节尺度上可能由横桥异步循环引起的结构涨落,其相对轴向速度必须小于3微米/秒或相对轴向位移小于0.05微米。