Department of Chemistry, California State University, Fresno, California.
Department of Biology, California State University, Fresno, California.
J Exp Zool A Ecol Integr Physiol. 2020 Jan;333(1):29-37. doi: 10.1002/jez.2318. Epub 2019 Sep 23.
The aquatic bladderwort Utricularia gibba captures zooplankton in mechanically triggered underwater traps. With characteristic dimensions <1 mm, the trapping structures are among the smallest known that work by suction-a mechanism that would not be effective in the creeping-flow regime. To understand the adaptations that make suction feeding possible on this small scale, we have measured internal flow speeds during artificially triggered feeding strikes in the absence of prey. These data are compared with complementary analytical models of the suction event: an inviscid model of the jet development in time and a steady-state model incorporating friction. The initial dynamics are well described by a time-dependent Bernoulli equation in which the action of the trap door is represented by a step increase in driving pressure. According to this model, the observed maximum flow speed (5.2 m/s) depends only on the pressure difference, whereas the initial acceleration (3 × 10 m/s ) is determined by pressure difference and channel length. Because the terminal speed is achieved quickly (0.2 ms) and the channel is short, the remainder of the suction event (2.0 ms) is effectively an undeveloped viscous steady state. The steady-state model predicts that only 17% of power is lost to friction. The energy efficiency and steady-state fluid speed decrease rapidly with decreasing channel diameter, setting a lower limit on practical bladderwort size.
水生狸藻通过机械触发的水下陷阱捕获浮游动物。具有 <1mm 的特征尺寸,这些陷阱结构是已知的通过吸力工作的最小结构之一——这种机制在缓流状态下是无效的。为了了解在这种小尺度下使吸力进食成为可能的适应机制,我们在没有猎物的情况下测量了人工触发进食时的内部流速。这些数据与吸力事件的补充分析模型进行了比较:一个是射流发展的时变无粘模型,另一个是包含摩擦的稳态模型。初始动力学很好地由一个时变伯努利方程描述,其中陷阱门的作用由驱动压力的阶跃增加来表示。根据该模型,观察到的最大流速(5.2m/s)仅取决于压差,而初始加速度(3×10m/s)由压差和通道长度决定。由于终端速度很快(0.2ms)且通道很短,因此吸力事件的其余部分(2.0ms)实际上是一个未发展的粘性稳态。稳态模型预测,只有 17%的能量损失于摩擦。能量效率和稳态流体速度随通道直径的减小而迅速下降,为实际狸藻大小设定了下限。