Fujime S, Ishiwata S, Maeda T
Biophys Chem. 1984 Aug;20(1-2):1-21. doi: 10.1016/0301-4622(84)80001-0.
By use of digital autocorrelation and fast Fourier methods, dynamic light-scattering studies of in vitro reconstituted muscle F-actin were made over a wide range of concentrations, 0.01-2 mg/ml F-actin. Measurements of correlation function [g1(t)]2 showed that a transition from a dilute to a semidilute regime for the Brownian motions of filaments occurred at around 0.3 mg/ml F-actin. Beyond this concentration, profiles of successively measured [g1(t)]2 showed very poor reproducibility. This resulted from the existence of very slow components, which could not be measured with a high statistical accuracy even for a measuring time of 3600 s/run. On the other hand, subtraction of these components automatically by an electronic circuit, [g-1(t)]2, or by computer processing, [g1(t)]2, resulted in a fairly good reproducibility of the profiles. The decay characteristics of [g1(t)]2 (and [g-1(t)]2) were very similar to those of [g1(t)]2 for dilute solutions. A theoretical model will be discussed which could account for the above situation. The time sequence [n(t,T)] of photoelectron counts at a sampling time T of light scattered from semidilute solutions of F-actin was stored on magnetic tapes, and both power spectra S(f) and correlation functions [g-1(t)]2 were computed by taking the ensemble average over many short records with duration 1024T. Since both S(f) and [g-1(t)]2 lacked frequency components lower than 1/(2048T) Hz, their profiles were highly reproducible. An analysis of S(f) confirmed our earlier results which had shown an apparent contradiction to later results by a correlation method. A comparison of S(f) and [g-1(t)]2 based on the same [n(t,T)] clarified the reasons why the bandwidth gamma of S(f) largely differed from the bandwidth gamma of [g1(t)]2 and [g-1(t)]2. The temperature dependence of gamma suggested that F-actin would be flexible and that the flexibility parameter would change with temperature.
通过使用数字自相关和快速傅里叶方法,在0.01 - 2mg/ml F - 肌动蛋白的广泛浓度范围内,对体外重构的肌肉F - 肌动蛋白进行了动态光散射研究。对相关函数[g1(t)]²的测量表明,对于细丝的布朗运动,从稀溶液到半稀溶液状态的转变发生在约0.3mg/ml F - 肌动蛋白处。超过此浓度,连续测量的[g1(t)]²的曲线显示出非常差的可重复性。这是由于存在非常缓慢的成分,即使每次测量时间为3600秒,也无法以高统计精度进行测量。另一方面,通过电子电路自动减去这些成分得到的[g - 1(t)]²,或通过计算机处理得到的[g1(t)]²,其曲线具有相当好的可重复性。[g1(t)]²(以及[g - 1(t)]²)的衰减特性与稀溶液中[g1(t)]²的衰减特性非常相似。将讨论一个理论模型,该模型可以解释上述情况。在从F - 肌动蛋白半稀溶液散射的光的采样时间T处的光电子计数的时间序列[n(t,T)]被存储在磁带上,并且通过对许多持续时间为1024T的短记录进行系综平均来计算功率谱S(f)和相关函数[g - 1(t)]²。由于S(f)和[g - 1(t)]²都缺乏低于1/(2048T)Hz的频率成分,它们的曲线具有高度可重复性。对S(f)的分析证实了我们早期的结果,这些结果与后来通过相关方法得到的结果明显矛盾。基于相同的[n(t,T)]对S(f)和[g - 1(t)]²进行比较,阐明了S(f)的带宽γ与[g1(t)]²和[g - 1(t)]²的带宽γ有很大差异的原因。γ的温度依赖性表明F - 肌动蛋白是灵活的,并且灵活性参数会随温度变化。