Pedley T J, Hill N A, Kessler J O
Department of Applied Mathematics and Theoretical Physics, University of Cambridge, UK.
J Fluid Mech. 1988;195:223-37. doi: 10.1017/s0022112088002393.
'Bioconvection' is the name given to pattern-forming convective motions set up in suspensions of swimming micro-organisms. 'Gyrotaxis' describes the way the swimming is guided through a balance between the physical torques generated by viscous drag and by gravity operating on an asymmetric distribution of mass within the organism. When the organisms are heavier towards the rear, gyrotaxis turns them so that they swim towards regions of most rapid downflow. The presence of gyrotaxis means that bioconvective instability can develop from an initially uniform suspension, without an unstable density stratification. In this paper a continuum model for suspensions of gyrotactic micro-organisms is proposed and discussed; in particular, account is taken of the fact that the organisms of interest are non-spherical, so that their orientation is influenced by the strain rate in the ambient flow as well as the vorticity. This model is used to analyse the linear instability of a uniform suspension. It is shown that the suspension is unstable if the disturbance wavenumber is less than a critical value which, together with the wavenumber of the most rapidly growing disturbance, is calculated explicitly. The subsequent convection pattern is predicted to be three-dimensional (i.e. with variation in the vertical as well as the horizontal direction) if the cells are sufficiently elongated. Numerical results are given for suspensions of a particular algal species (Chlamydomonas nivalis); the predicted wavelength of the most rapidly growing disturbance is 5-6 times larger than the wavelength of steady-state patterns observed in experiments. The main reasons for the difference are probably that the analysis describes the onset of convection, not the final, nonlinear steady state, and that the experimental fluid layer has finite depth.
“生物对流”是指在游动微生物悬浮液中形成的模式形成对流运动。“回转趋性”描述了游动过程通过粘性阻力产生的物理扭矩与作用于生物体质量不对称分布上的重力之间的平衡来引导的方式。当生物体后部较重时,回转趋性会使它们转向,从而朝着下降最快的区域游动。回转趋性的存在意味着生物对流不稳定性可以从初始均匀的悬浮液中发展而来,而无需不稳定的密度分层。本文提出并讨论了一个用于回转趋性微生物悬浮液的连续介质模型;特别地,考虑到所关注的生物体是非球形的这一事实,因此它们的取向受周围流体中的应变率以及涡度的影响。该模型用于分析均匀悬浮液的线性不稳定性。结果表明,如果扰动波数小于一个临界值,则悬浮液是不稳定的,该临界值与增长最快的扰动的波数一起被明确计算出来。如果细胞足够细长,预计随后的对流模式将是三维的(即在垂直方向以及水平方向上都有变化)。给出了一种特定藻类(雪衣藻)悬浮液的数值结果;预测的增长最快的扰动的波长比实验中观察到的稳态模式的波长大约5 - 6倍。差异的主要原因可能是该分析描述的是对流的起始,而非最终的非线性稳态,并且实验流体层具有有限深度。