Brokaw C J
Biophys J. 1985 Oct;48(4):633-42. doi: 10.1016/S0006-3495(85)83819-4.
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.
计算机模拟用于研究一个简单的鞭毛模型,该模型在没有粘性阻力的情况下能够启动并传播弯曲波。该模型仅包含弹性弯曲阻力和一个主动滑动机制,该机制随着滑动速度的增加而产生减小的主动剪切力矩。振荡源于一种分布式控制机制,当曲率在任一方向达到临界值时,该机制会反转主动滑动机制的运行方向。因此,由曲率控制的鞭毛模型进行的弯曲传播不需要与外部流体的粘性阻力相互作用。对该模型在弯曲传播过程中的力矩平衡进行分析研究,得出一条解曲线,该曲线给出了满足力矩平衡方程并实现均匀弯曲传播的频率和波长值,这表明该模型是欠定的。在零粘度时,新弯曲形成过程中鞭毛基部末端零剪切速率的边界条件选择了通过计算机模拟获得的特定解。因此,鞭毛基部末端弯曲起始模式的细节对于确定鞭毛远端部分传播的弯曲波的特性可能具有重要意义。在高外部粘度值下,该模型以在鞭毛上产生近似整数波数的频率和波长振荡。选择这些工作点是因为它们有助于在模型末端平衡弯矩,在这些末端外部粘性力矩接近零。通过迫使模型以预定频率运行,可以 override 这些模式偏好。与真实鞭毛显示的弱模式偏好或无模式偏好相比由曲率控制的鞭毛模型显示的强模式偏好,因此并不能证明力矩平衡方法对真实鞭毛不适用。相反,它们表明需要指定真实鞭毛的其他属性,这些属性负责选择特定的工作点。