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相关概念视频

Viscosity01:17

Viscosity

5.7K
When water is poured into a glass, it falls freely and quickly, whereas if honey or maple syrup is poured over a pancake, it flows slowly and sticks to the surface of the container. This difference in the flow of different kinds of liquids arises due to the fluid friction between the liquid layers and the liquid and the surrounding material. This property of fluids is called fluid viscosity. In this example, water has a lower viscosity than honey and maple syrup.
The SI unit of viscosity is...
5.7K
Types of Fluids01:27

Types of Fluids

118
Fluids can be classified into Newtonian and non-Newtonian fluids based on their response to shear stress. Newtonian fluids have a linear relationship between shear stress and the shear strain rate, following Newton's law of viscosity. Their viscosity remains constant regardless of the shear rate, making their behavior predictable and easier to analyze. Common examples include water, air, oil, and gasoline.
In contrast, non-Newtonian fluids do not follow Newton's law of viscosity, and...
118
Surface Tension, Capillary Action, and Viscosity02:57

Surface Tension, Capillary Action, and Viscosity

27.3K
Surface Tension
The various IMFs between identical molecules of a substance are examples of cohesive forces. The molecules within a liquid are surrounded by other molecules and are attracted equally in all directions by the cohesive forces within the liquid. However, the molecules on the surface of a liquid are attracted only by about one-half as many molecules. Because of the unbalanced molecular attractions on the surface molecules, liquids contract to form a shape that minimizes the number...
27.3K
Thin-Walled Hollow Shafts01:15

Thin-Walled Hollow Shafts

155
In analyzing a thin-walled hollow shaft subjected to torsional loading, a segment with width dx is isolated for examination. Despite its equilibrium state, this segment faces torsional shearing forces at its ends. These forces are quantitatively described by the product of the longitudinal shearing stress on the segment's minor surface and the area of this surface, leading to the concept of shear flow. This shear flow is consistent throughout the structure, indicating a uniform distribution...
155
Frictional Force01:07

Frictional Force

6.7K
When a body is in motion, it encounters resistance because the body interacts with its surroundings. This resistance is known as friction, a common yet complex force whose behavior is still not completely understood. Friction opposes relative motion between systems in contact, but also allows us to move. Friction arises in part due to the roughness of surfaces in contact. For one object to move along a surface, it must rise to where the peaks of the surface can skip along the bottom of the...
6.7K
Viscosity of Fluid01:19

Viscosity of Fluid

225
Viscosity measures the resistance a fluid offers to flow and deformation. It results from internal friction between layers of fluid moving relative to one another. Dynamic viscosity, denoted by the Greek letter mu (μ), quantifies the force needed to move one fluid layer over another. For Newtonian fluids like water and air, the relationship between the shearing stress and the rate of shearing strain is linear, meaning their viscosity remains constant regardless of the applied stress.
225

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相关实验视频

Updated: May 14, 2025

Experimental Measurement of Settling Velocity of Spherical Particles in Unconfined and Confined Surfactant-based Shear Thinning Viscoelastic Fluids
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Experimental Measurement of Settling Velocity of Spherical Particles in Unconfined and Confined Surfactant-based Shear Thinning Viscoelastic Fluids

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积极的萨夫曼-泰勒粘性指纹

Akash Ganesh1, Carine Douarche1, Harold Auradou1

  • 1FAST, Université Paris-Saclay, CNRS, 91405 Orsay, France.

Physical review letters
|April 11, 2025
PubMed
概括

在液体中游泳的细菌可以将其粘度降低到零,在流体移动过程中创建复杂的,类似手指的模式. 这种不稳定性发生在细菌度和剪切速率的特定条件下.

科学领域:

  • 流体动力学 流体动力学
  • 微生物学 微生物学
  • 类风病学 类风病学 类风病学

背景情况:

  • 游泳的微生物可以改变液体的大量性质.
  • 在细菌悬浮液中有效切割粘度降至零是一个已知的现象.
  • 经典的萨夫曼-泰勒不稳定性描述了简单的流体系统中的粘性指纹.

研究的目的:

  • 调查细菌悬浮物的零粘度特性是否会导致粘性指纹.
  • 描述这些系统中流体移位前线的动态行为.
  • 确定不稳定性发生的条件.

主要方法:

  • 对流体移位前线的实验观测.
  • 系统地改变细菌体积分数和强加的剪切速率.
  • 对由此产生的动态特征和不稳定形成的分析.

主要成果:

  • 该系统表现出复杂的动态特征,超出了经典的萨夫曼-泰勒不稳定性.
  • 观察到粘性类似手指的位移前线.
  • 当细菌体积分数超过临界值,剪切率低于临界值时,不稳定性发生,与零粘度相吻合.

结论:

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Preparation and Friction Force Microscopy Measurements of Immiscible, Opposing Polymer Brushes

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Fabricating High-viscosity Droplets using Microfluidic Capillary Device with Phase-inversion Co-flow Structure
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Fabricating High-viscosity Droplets using Microfluidic Capillary Device with Phase-inversion Co-flow Structure

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Experimental Measurement of Settling Velocity of Spherical Particles in Unconfined and Confined Surfactant-based Shear Thinning Viscoelastic Fluids
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Experimental Measurement of Settling Velocity of Spherical Particles in Unconfined and Confined Surfactant-based Shear Thinning Viscoelastic Fluids

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Preparation and Friction Force Microscopy Measurements of Immiscible, Opposing Polymer Brushes
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Preparation and Friction Force Microscopy Measurements of Immiscible, Opposing Polymer Brushes

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Fabricating High-viscosity Droplets using Microfluidic Capillary Device with Phase-inversion Co-flow Structure
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Fabricating High-viscosity Droplets using Microfluidic Capillary Device with Phase-inversion Co-flow Structure

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  • 呈现有效粘度为零的细菌悬浮物可以导致复杂的流体移位模式.
  • 观察到的不稳定性与经典的萨夫曼-泰勒不稳定性不同.
  • 临界细菌度和剪切率是不稳定性开始的关键参数.