Wormlike Chains Near the Rod Limit: Translational Friction Coefficient
Wormlike Chains Near the Rod Limit: Translational Friction Coefficient
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DOI:
10.1021/ma60068a032
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发表时间:
1979-03
期刊:
影响因子:
5.5
通讯作者:
T. Norisuye;M. Motowoka;H. Fujita
中科院分区:
文献类型:
--
作者:
T. Norisuye;M. Motowoka;H. Fujita
The translational friction coefficient,, of the Kratky-Porod (KP) wormlike chain near the rod limit is calculated according to the Yamakawa-Fujii formulation of the Oseen-Burgers method, with a wormlike sausage model assumed for the chain. Here wormlike sausage means a wormlike cylinder capped with hemispheres at its ends. The resulting expression for converges to the Stokes law at the limit of L= d, where L is the contour length and d is the diameter of the sausage. Its comparison with the Yamakawa-Fujii expression, which ignores end effects, shows that end corrections to are unexpectedly small. In fact, the Yamakawa-Fujii theory is accurate down to as short a chain as L/d~ 4.Among others, 1™ 5 the most accurate formulation of the translational friction coefficient,, of the Kratky-Porod wormlike chain6 (KP chain) is one worked out by Ya-makawa and Fujii5 with a model that theycall the wormlike cylinder. However, it is still incomplete in that it neglects contributions from the ends of the cylinder. Judging from a study by Broersma7 on straight cylinders, one may anticipate that end effects on hydrodynamic behavior should become significant as the KP chain gets shorter. The purpose of the present paper is to estimate such effects on, using a wormlike sausage model for the KP chain. This model is a wormlike cylinder capped with two hemispheres at its ends, as illustrated in Figure 1. It is assumed that the central axis of the sausage has a flexibility characteristic of the KP chain. We also assume that the cross-section of each hemisphere perpendicular to the central axis stays circular in whatever way the sausage is deformed. Our calculation will be restricted to the sausage near the rod limit, because by so doing the previously derived moments8 (R2m (R* u0) n)(m, n=