通过空间调制来混合流体的工程性质.
1Department of Engineering Science, University of Electro-Communications, Tokyo 182-8585, Japan.
Physical review letters
|May 10, 2024
概括
我们开发了一种新的方法来控制使用外部潜力的流体混合. 这种技术允许在稀释的玻色子气体中进行可调节的相互作用,从而导致新的相位行为,如混合泡状态.
科学领域:
- 量子物理学的量子物理学
- 统计力学就是统计力学.
- 流体动力学 流体动力学
背景情况:
- 控制流体间相互作用对于理解相位过渡至关重要.
- 外部潜能提供了一种在微观水平上操纵物质的方法.
研究的目的:
- 引入一种用于控制流体混合特性的新方法.
- 为了研究在外部周期潜力下稀释玻色子气体的相位行为.
主要方法:
- 使用外部周期电位调节两个流体的局部密度分布.
- 将该方法应用于稀释玻色子气体的混合物.
- 分析相位图,包括双极和旋极曲线.
主要成果:
- 证明了对有效的流体相互作用和混合性能的控制.
- 在相位图中观察到双节曲线和旋节曲线的出现.
- 实现了螺旋体分解到混合泡状态,具有有限的混合比率.
- 实现了通过核化表现相分离的转移稳定混合物.
结论:
- 外部周期电位为调整流体相互作用和相位行为提供了强大的工具.
- 拟议的方法可以创建新的物质状态,例如混合泡阶段.
- 这种方法为控制量子系统中的相位分离开辟了新的途径.
相关概念视频
Types of Fluids
237
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...
In contrast, non-Newtonian fluids do not follow Newton's law of viscosity, and...
237
Characteristics of Fluids
3.9K
When a force is applied parallel to the top surface of a solid, it resists the applied force due to the internal frictional forces between the layers of the solid known as shearing resistance. However, when the force is removed, the shearing forces restore the original shape of the solid. Other deformation forces also cause temporary changes in shape if the forces are not beyond a threshold magnitude. Solids tend to retain their shape, making the study of their rest and motion easier. Beyond...
3.9K
Accelerating Fluids
1.0K
When a fluid is in constant acceleration, the pressure and buoyant force equations are modified. Suppose a beaker is placed in an elevator accelerating upward with a constant acceleration, a. In the beaker, assume there is a thin cylinder of height h with an infinitesimal cross-sectional area, ΔS.
The motion of the liquid within this infinitesimal cylinder is considered to obtain the pressure difference. Three vertical forces act on this liquid:
The motion of the liquid within this infinitesimal cylinder is considered to obtain the pressure difference. Three vertical forces act on this liquid:
1.0K
Laminar and Turbulent Flow
8.5K
Fluid dynamics is the study of fluids in motion. Velocity vectors are often used to illustrate fluid motion in applications like meteorology. For example, wind—the fluid motion of air in the atmosphere—can be represented by vectors indicating the speed and direction of the wind at any given point on a map. Another method for representing fluid motion is a streamline. A streamline represents the path of a small volume of fluid as it flows. When the flow pattern changes with time, the...
8.5K
Pressure Variation in a Fluid at Rest
248
In a fluid at rest, the pressure at any point beneath the fluid surface depends solely on the depth, not on the container's shape or size. This principle, known as hydrostatic pressure, arises because, in stationary fluids, there is no acceleration, meaning the forces within the fluid balance out. Only vertical forces, caused by the weight of the fluid above, contribute to pressure changes with depth.
When measuring pressure at two different levels within the fluid, the difference in...
When measuring pressure at two different levels within the fluid, the difference in...
248
Viscosity of Fluid
392
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.
392


