在由摩西效应控制的液体-空气界面上,詹纳斯球形粒子的运动和方向
Abhishek Kaushal1,2, Oleg Gendelman3, Shraga Shoval2
1Engineering Faculty, Chemical Engineering Department, Ariel University, Ariel 407000, Israel.
Langmuir : the ACS journal of surfaces and colloids
|August 6, 2024
概括
磁性Janus粒子和聚乙烯粒子在盐水接口上向磁场移动. 一个新的框架解释了它们的运动,受磁力,引力和毛细血管力的影响,具有自我组装的潜力.
科学领域:
- 物理 物理学 物理
- 材料科学 材料科学 材料科学
- 体科学 体科学 体科学
背景情况:
- 具有磁性涂层的Janus粒子表现出独特的界面行为.
- 了解液体-空气接口上的粒子运动对于自组装应用至关重要.
- 磁场可以用来操纵界面上的微观物体.
研究的目的:
- 为了研究磁场下的空气/盐水接口上的磁性Janus粒子的运动.
- 为了将它们的运动与纯聚乙烯粒子进行比较.
- 开发一个理论框架来解释观察到的粒子动态.
主要方法:
- 在0.5 T磁场下对粒子运动的实验观测.
- 在不同的磁场强度和盐度下分析粒子移位.
- 开发一个结合磁力,引力和毛细血管力的理论模型.
主要成果:
- 雅努斯和聚乙烯颗粒都向磁铁移动,并停在磁场诱导的井上.
- 运动受到摩西效应,磁场强度和盐度的影响.
- 开发了一个统一的理论框架,突出了磁能,接口曲率,重力和毛细血管力的相互作用.
结论:
- 空气 - 盐溶液界面上的粒子运动是由复杂的力量相互作用决定的,而不仅仅是磁能.
- 开发的框架为观察到的现象提供了定性解释.
- 这项研究表明了在液体/空气接口上的粒子自组装的潜在应用.
相关概念视频
Surface Tension of Fluid
255
Surface tension is a fundamental property of fluids, occurring at the boundary between a liquid and a gas or between two immiscible liquids. This phenomenon arises from the cohesive forces between molecules at the fluid's surface, creating an effect similar to a stretched elastic membrane. Inside each fluid, molecules are equally attracted in all directions by neighboring molecules, but surface molecules experience a net inward force, resulting in surface tension.
Surface tension varies...
Surface tension varies...
255
Surface Tension, Capillary Action, and Viscosity
27.7K
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...
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...
27.7K
Contact Angle
12.3K
When a solid is dipped inside a liquid, the liquid surface becomes curved near the contact. For some solid–liquid interfaces, the liquid is pulled up along the solid, while for others, the liquid surface is convex or depressed near the solid surface. This phenomenon can be explained using the concept of cohesive and adhesive forces.
The adhesive force is the molecular force between molecules of different materials, that is, between the molecules of the solid and the liquid. The cohesive...
The adhesive force is the molecular force between molecules of different materials, that is, between the molecules of the solid and the liquid. The cohesive...
12.3K
Fluid Mosaic Model
11.5K
Scientists identified the plasma membrane in the 1890s and its principal chemical components (lipids and proteins) by 1915. The model for plasma membrane structure, proposed in 1935 by Hugh Davson and James Danielli, was the first model to be widely accepted in the scientific community. The model was based on the plasma membrane's "railroad track" appearance in early electron micrographs. Davson and Danielli theorized that the plasma membrane's structure resembled a sandwich...
11.5K
The Fluid Mosaic Model
146.3K
The fluid mosaic model was first proposed as a visual representation of research observations. The model comprises the composition and dynamics of membranes and serves as a foundation for future membrane-related studies. The model depicts the structure of the plasma membrane with a variety of components, which include phospholipids, proteins, and carbohydrates. These integral molecules are loosely bound, defining the cell’s border and providing fluidity for optimal function.
146.3K
Viscosity of Fluid
371
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.
371


