Schmidt F G, Hinner B, Sackmann E, Tang J X
Technische Universität München, Institut für Biophysik E22, James-Franck- Strasse, D-85747 München, Germany.
Phys Rev E Stat Phys Plasmas Fluids Relat Interdiscip Topics. 2000 Oct;62(4 Pt B):5509-17. doi: 10.1103/physreve.62.5509.
The cytoskeletal protein filament F-actin has been treated in a number of recent studies as a model physical system for semiflexible filaments. In this work, we studied the viscoelastic properties of entangled solutions of the filamentous bacteriophage fd as an alternative to F-actin with similar physical parameters. We present both microrheometric and macrorheometric measurements of the viscoelastic storage and loss moduli, G'(f ) and G"(f ), respectively, in a frequency range 0.01<f<4 Hz, for fd solutions in the concentration range 5<c<15 mg/ml. The onset of a narrow and slanted plateaulike region of G'(f ) is located at around 2 Hz. The variation of the plateau modulus with concentration obeys a power law G(')(N) approximately c(1.4+/-0.3), similar to that found for entangled solutions of F-actin. In the low-frequency regime, the frequency dependence of the viscoelastic moduli can be described by power laws G'(f ) approximately f(0.9-1.2) and G"(f ) approximately f(0.7-0.9), which deviate significantly from the simple theoretical predictions of G'(f ) approximately f(2) and G"(f ) approximately f(1). The latter behavior cannot yet be understood within the framework of current theories of semiflexible filament networks. For the dynamic viscosity at the low shear rate limit, a concentration dependence of eta(0) approximately c(2.6) was found. Finally, a linear scaling of the terminal relaxation time with concentration, tau(d) approximately c, was observed.
细胞骨架蛋白丝F-肌动蛋白在最近的一些研究中被当作半柔性丝的一个典型物理系统。在这项工作中,我们研究了丝状噬菌体fd缠结溶液的粘弹性性质,以此作为具有相似物理参数的F-肌动蛋白的替代物。我们给出了在0.01<f<4 Hz频率范围内,浓度为5<c<15 mg/ml的fd溶液的粘弹性储能模量G'(f)和损耗模量G"(f)的微观流变学和宏观流变学测量结果。G'(f)的一个狭窄且倾斜的平台状区域的起始点位于约2 Hz处。平台模量随浓度的变化服从幂律G(')(N)约为c(1.4±0.3),这与F-肌动蛋白缠结溶液的情况类似。在低频区域,粘弹性模量的频率依赖性可用幂律G'(f)约为f(0.9 - 1.2)和G"(f)约为f(0.7 - 0.9)来描述,这与G'(f)约为f(2)和G"(f)约为f(1)的简单理论预测有显著偏差。后一种行为在当前半柔性丝网络理论的框架内还无法得到解释。对于低剪切速率极限下的动态粘度,发现其浓度依赖性为eta(0)约为c(2.6)。最后,观察到终端弛豫时间与浓度呈线性比例关系,tau(d)约为c。