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Computer simulation of flagellar movement. VI. Simple curvature-controlled models are incompletely specified.

机译:鞭毛运动的计算机模拟。 VI。未完全指定简单的曲率控制模型。

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摘要

Computer simulation is used to examine a simple flagellar model that will initiate and propagate bending waves in the absence of viscous resistances. The model contains only an elastic bending resistance and an active sliding mechanism that generates reduced active shear moment with increasing sliding velocity. Oscillation results from a distributed control mechanism that reverses the direction of operation of the active sliding mechanism when the curvature reaches critical magnitudes in either direction. Bend propagation by curvature-controlled flagellar models therefore does not require interaction with the viscous resistance of an external fluid. An analytical examination of moment balance during bend propagation by this model yields a solution curve giving values of frequency and wavelength that satisfy the moment balance equation and give uniform bend propagation, suggesting that the model is underdetermined. At 0 viscosity, the boundary condition of 0 shear rate at the basal end of the flagellum during the development of new bends selects the particular solution that is obtained by computer simulations. Therefore, the details of the pattern of bend initiation at the basal end of a flagellum can be of major significance in determining the properties of propagated bending waves in the distal portion of a flagellum. At high values of external viscosity, the model oscillates at frequencies and wavelengths that give approximately integral numbers of waves on the flagellum. These operating points are selected because they facilitate the balance of bending moments at the ends of the model, where the external viscous moment approaches 0. These mode preferences can be overridden by forcing the model to operate at a predetermined frequency. The strong mode preferences shown by curvature-controlled flagellar models, in contrast to the weak or absent mode preferences shown by real flagella, therefore do not demonstrate the inapplicability of the moment-balance approach to real flagella. Instead, they indicate a need to specify additional properties of real flagella that are responsible for selecting particular operating points.
机译:使用计算机仿真来检查简单的鞭毛模型,该模型将在没有粘性阻力的情况下引发并传播弯曲波。该模型仅包含弹性弯曲阻力和主动滑动机制,该机制随滑动速度的增加而产生减小的主动剪切力矩。振荡是由分布式控制机构产生的,当曲率在任一方向上达到临界值时,该控制机构会反转主动滑动机构的操作方向。因此,曲率控制的鞭毛模型的弯曲传播不需要与外部流体的粘性阻力相互作用。通过此模型对弯矩传播过程中的力矩平衡进行分析检查,得出一条解曲线,给出了满足矩平衡方程并给出均匀弯矩传播的频率和波长值,这表明该模型尚未确定。在粘度为0时,在新弯曲形成过程中鞭毛基端的剪切速率为0的边界条件选择了通过计算机模拟获得的特定解决方案。因此,在确定鞭毛远侧部分中传播的弯曲波的特性时,在鞭毛基端弯曲开始的模式的细节可能具有重要意义。在较高的外部粘度值下,模型会在鞭毛上产生大约整数倍波数的频率和波长下振荡。选择这些工作点是因为它们有助于在模型的末端(外部粘性力矩接近0)平衡弯矩。可以通过强制模型以预定频率运行来覆盖这些模式首选项。与真实鞭毛所显示的弱模式偏好或不存在模式偏好相比,曲率控制鞭毛模型所显示的强模式偏好,因此没有证明力矩平衡方法不适用于真实鞭毛。相反,它们指示需要指定真正的鞭毛的其他属性,这些属性负责选择特定的操作点。

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