相关实验视频
Updated: Jul 5, 2025

08:43
Calibration Procedures for Orthogonal Superposition Rheology
Published on: November 18, 2020
2.1K
使用OrthoBoXY方法计算精确的真实自我扩散系数和剪切粘度
Johanna Busch1, Dietmar Paschek1
1Institut für Chemie, Abteilung Physikalische und Theoretische Chemie, Universität Rostock, Albert-Einstein-Str. 27, D-18059 Rostock, Germany.
The journal of physical chemistry. B
|January 19, 2024
概括
本研究介绍了OrthoBoXY方法用于分子动力学模拟,使得自我扩散和粘度的准确计算. 这些发现表明,较长的模拟时间比较大的系统大小更有效,以获得可靠的数据.
科学领域:
- 计算化学计算化学
- 材料科学 材料科学 材料科学
- 物理化学 物理化学
背景情况:
- 分子动力学 (MD) 模拟对于理解材料特性至关重要.
- 准确计算自我扩散系数和粘度对于各种应用至关重要.
- 系统大小和模拟长度会影响MD模拟结果的可靠性.
研究的目的:
- 验证OrthoBoXY方法用于计算自扩散系数和剪切粘度.
- 评估OrthoBoXY方法在各种化学系统中的效率.
- 为优化MD模拟参数提供指导方针,以获得可靠的数据.
主要方法:
- 应用OrthoBoXY方法与特定的正方形周期边界条件.
- 在各种系统上测试方法,包括水,,混合物和离子液体.
- 分析系统大小和模拟长度对统计不确定性的依赖.
主要成果:
- 在OrthoBoXY方法准确地确定真正的自我扩散系数 (D0) 和剪切粘度.
- 对于特定的盒子比率,扩散系数的系统大小独立性得到证实.
- 延长模拟长度比增加系统大小更有利于减少不确定性.
结论:
- 在计算可靠的自我扩散和粘度数据时,OrthoBoXY方法是有效的.
- 用大约768个分子或离子对进行的MD模拟足够.
- 优先考虑模拟长度而不是系统大小,可以确保MD研究中的数据可靠性.
相关概念视频
Viscosity of Fluid
421
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.
421
Thin-Walled Hollow Shafts
192
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...
192
Navier–Stokes Equations
507
For incompressible Newtonian fluids, where density remains constant, stresses show a linear relationship with the deformation rate, defined by normal and shear stresses. Normal stresses depend on the pressure exerted on the fluid and the rate of deformation in specific directions, which determines how fluid flows under varying pressures. Shear stresses, on the other hand, act tangentially across fluid layers. They explain how adjacent fluid layers slide relative to one another, connecting...
507
Viscosity
5.9K
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...
The SI unit of viscosity is...
5.9K
Divergence and Stokes' Theorems
1.6K
The divergence and Stokes' theorems are a variation of Green's theorem in a higher dimension. They are also a generalization of the fundamental theorem of calculus. The divergence theorem and Stokes' theorem are in a way similar to each other; The divergence theorem relates to the dot product of a vector, while Stokes' theorem relates to the curl of a vector. Many applications in physics and engineering make use of the divergence and Stokes' theorems, enabling us to write...
1.6K
Newtonian Fluid: Problem Solving
227
Newtonian fluids exhibit a constant viscosity, meaning their shear stress and shear strain rate are directly proportional. This property ensures a predictable and stable response to applied forces, maintaining a linear relationship between force and flow. Examples include water, air, and light oils, consistently demonstrating this proportional behavior regardless of external conditions.
A velocity gradient forms within the fluid when a Newtonian fluid is placed between two parallel plates, with...
A velocity gradient forms within the fluid when a Newtonian fluid is placed between two parallel plates, with...
227

