相关实验视频
Updated: Jan 17, 2026

08:37
Forming, Confining, and Observing Microtubule-Based Active Nematics
Published on: January 13, 2023
3.1K
活体体质中的自发流:由环状封闭诱导的效应.
A Aramini1, G Napoli2, S Turzi3
1Università del Salento, Dipartimento di Matematica e Fisica "E. De Giorgi", Lecce, Italy.
Physical review. E
|September 16, 2025
概括
这项研究探讨了活体阴性材料如何在曲的空间中流动. 域曲率和面积比影响自发流动,环形域显示独特的双带配置.
科学领域:
- 物理 物理学 物理
- 材料科学 材料科学 材料科学
- 流体动力学 流体动力学
背景情况:
- 活跃的敌人表现出由内部压力驱动的自发流动.
- 狭窄的几何形状显著改变了活性材料的流动动力学.
研究的目的:
- 为了研究活动诱导的线状流在环状域内的活性阴性体中.
- 分析域几何学的作用,特别是曲率和面积比,在流动启动和配置上.
主要方法:
- 问题作为非线性边界值问题的表述.
- 控制方程的分支分析,以确定关键值.
- 在不同的活动和曲率参数下,研究流动模式.
主要成果:
- 自发流动启动的临界值取决于域的尺寸比.
- 域曲率降低了临界值,并解决了平面几何体中看到的流动不确定性.
- 环形域表现出具有最低激活值的双带配置,过渡到单向流与增加的活动或曲率.
结论:
- 域几何学对于控制活跃的阴性流动模式至关重要.
- 这些发现提供了关于活体物质在狭窄,曲的环境中的行为,与生物系统相关的见解.
相关概念视频
Couette Flow
956
Couette flow represents the flow of fluid between two parallel plates, with one plate fixed and the other moving with a constant velocity. This configuration allows for a simplified analysis using the Navier-Stokes equations, which govern fluid motion under conditions of viscosity and incompressibility. For Couette flow, the assumptions include a steady, laminar, incompressible flow with a zero-pressure gradient in the flow direction. This flow type is beneficial for understanding shear-driven...
956
Steady, Laminar Flow Between Parallel Plates
797
Understanding steady, laminar flow between parallel plates is essential for analyzing and designing flow in narrow rectangular channels, commonly found in various water conveyance and drainage systems. The Navier-Stokes equations govern fluid motion and are generally challenging to solve due to their nonlinearity. However, simplifications are possible in certain cases, like the steady laminar flow between parallel plates. For this scenario, we assume steady, incompressible, laminar flow.
797
Irrotational Flow
947
Irrotational flow is characterized by fluid motion where particles do not rotate around their axes, resulting in zero vorticity. For a flow to be irrotational, the curl of the velocity field must be zero. This imposes specific conditions on velocity gradients. For instance, to maintain zero rotation about the z-axis, the gradient condition:
947
Steady, Laminar Flow in Circular Tubes
1.0K
Hagen-Poiseuille flow describes a viscous fluid's steady, incompressible flow through a cylindrical tube with a constant radius R. This flow profile is often applied to understand fluid transport in narrow channels, such as capillaries. It serves as a foundational example of laminar flow. In this model, cylindrical coordinates (r,θ,z) are used to describe the radial (r), angular (θ), and axial (z) dimensions within the tube. For Hagen-Poiseuille flow, the velocity profile is purely axial,...
1.0K
Bernoulli's Equation for Flow Normal to a Streamline
1.3K
Bernoulli's equation for flow normal to a streamline explains how pressure varies across curved streamlines due to the outward centrifugal forces induced by the fluid's curvature. The pressure is higher on the inner side of the curve, near the center of curvature, and decreases outward to balance these centrifugal forces.
The pressure difference depends on the fluid's velocity and radius of curvature. The pressure variation is minimal in flows with nearly straight streamlines. However, the...
The pressure difference depends on the fluid's velocity and radius of curvature. The pressure variation is minimal in flows with nearly straight streamlines. However, the...
1.3K
Bernoulli's Equation for Flow Along a Streamline
1.4K
Bernoulli's equation relates the energy conservation in a fluid moving along a streamline. The equation applies to incompressible and inviscid fluids under steady flow. For such a flow, Newton's second law is applied to a small fluid element, which experiences forces due to pressure differences, gravity, and velocity variations. The force balance leads to the following form of Bernoulli's equation:
1.4K

