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Wrinkling Dynamics of Fluctuating Vesicles in Time-Dependent Viscous Flow

机译:随时间变化的粘性流中脉动囊泡的起皱动力学

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摘要

We study the fully nonlinear, nonlocal dynamics of two-dimensional vesicles in a time-dependent, incompressible viscous flow at finite temperature. We focus on a transient instability that can be observed when the direction of applied flow is suddenly reversed, which induces compressive forces on the vesicle interface, and small-scale interface perturbations known as wrinkles develop. These wrinkles are driven by regions of negative elastic tension on the membrane. Using a stochastic immersed boundary method with a biophysically motivated choice of thermal fluctuations, we investigate the wrinkling dynamics numerically. Different from deterministic wrinkling dynamics, thermal fluctuations lead to symmetry-breaking wrinkling patterns by exciting higher order modes. This leads to more rapid and more realistic wrinkling dynamics. Our results are in excellent agreement with the experimental data by Kantsler et al. We compare the nonlinear simulation results with perturbation theory, modified to account for thermal fluctuations. The strength of the applied flow strongly influences the most unstable wavelength characterizing the wrinkles, and there are significant differences between the results from perturbation theory and the fully nonlinear simulations, which suggests that the perturbation theory misses important nonlinear interactions. Strikingly, we find that thermal fluctuations actually have the ability to attenuate variability of the characteristic wavelength of wrinkling by exciting a wider range of modes than the deterministic case, which makes the evolution less constrained and enables the most unstable wavelength to emerge more readily. We further find that thermal noise helps prevent the vesicle from rotating if it is misaligned with the direction of the applied extensional flow.
机译:我们研究了在有限温度下随时间变化的不可压缩粘性流中二维囊泡的完全非线性,非局部动力学。我们关注的是瞬态不稳定性,当施加的流动方向突然反转时,可以观察到这种不稳定性,这会在囊泡界面上产生压缩力,从而形成小规模的界面扰动,称为皱纹。这些皱纹是由膜上的负弹性张力区域驱动的。使用随机浸没边界方法和热波动的生物物理动机选择,我们在数值上研究了起皱动力学。与确定性起皱动力学不同,热涨落通过激发高阶模态导致对称性破坏起皱。这导致更迅速和更现实的起皱动态。我们的结果与Kantsler等人的实验数据非常吻合。我们将非线性仿真结果与微扰理论进行比较,并对其进行了修正以解决热波动问题。施加的流动的强度极大地影响了表征皱纹的最不稳定波长,并且扰动理论和完全非线性模拟的结果之间存在显着差异,这表明扰动理论忽略了重要的非线性相互作用。令人惊讶地,我们发现,与确定性情况相比,热涨落实际上具有通过激发更宽范围的模式来减弱起皱特征波长的变化的能力,这使演化受到的约束更少,并使最不稳定的波长更容易出现。我们进一步发现,如果与所施加的拉伸流的方向未对准,则热噪声有助于防止囊泡旋转。

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