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相关概念视频

Boundary Conditions for Current Density01:25

Boundary Conditions for Current Density

932
Current density becomes discontinuous across an interface of materials with different electrical conductivities. The normal component of the current density is continuous across the boundary.
932
Continuity Equation01:20

Continuity Equation

933
The total amount of current flowing per unit cross-sectional area is called the current density. Hence, the current passing through a cross-sectional area can be written as the surface integral of the current density.
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Current Density01:21

Current Density

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The total amount of current flowing through one unit value of a cross-sectional area is referred to as current density. If the current flow is uniform, the amount of current flowing through a conductor is the same at all points along the conductor, even if the conductor area varies. The current density consists of the local magnitude and direction of the charge flow, which varies from point to point. Current density is measured in amperes per meter square, and direction is defined as the net...
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Energy Associated With a Charge Distribution01:21

Energy Associated With a Charge Distribution

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The work done to bring a charge through a distance r is given by the potential difference between the initial and the final position. To assemble a collection of point charges, the total work done can be expressed in terms of the product of each pair of charges divided by their separation distance, defined with respect to a suitable origin. Solving this expression gives the energy stored in a point charge distribution.
1.6K
Dry Friction01:30

Dry Friction

436
Dry friction occurs between two solid surfaces in contact as they attempt to move relative to one another. In daily life, dry friction is encountered in various forms, such as when walking on the ground, sliding an object across a table, or rubbing hands together. Despite its ubiquity, the underlying mechanisms behind dry friction are not readily visible.
To illustrate this concept, imagine a wooden crate resting on a rough, non-uniform horizontal surface. When an external force is applied to...
436
Frictional Force01:07

Frictional Force

8.2K
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...
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相关实验视频

Updated: Aug 9, 2025

Evolution of Staircase Structures in Diffusive Convection
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电荷密度演变 控制界面摩擦

Junhui Sun1,2, Xin Zhang1, Shiyu Du3,4

  • 1School of Mechanical Engineering, State Key Laboratory of Traction Power, Southwest Jiaotong University, Chengdu 610031, China.

Journal of the American Chemical Society
|February 22, 2023
PubMed
概括
此摘要是机器生成的。

表面摩擦源于电子屏障在滑动过程中抵抗原子重排. 这项研究揭示了摩擦能耗与电子进化之间的线性关系,为剪切强度和接触力学提供了洞察力.

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科学领域:

  • 表面科学
  • 部落学
  • 凝聚物质物理学

背景情况:

  • 固体的电子性质显著影响接触系统的特性.
  • 在界面摩擦中控制电子合的一般规则尚未确立.
  • 了解表面摩擦对于材料科学和纳米技术至关重要.

研究的目的:

  • 研究固体界面中的摩擦的物理起源.
  • 建立基于电子相互作用的界面摩擦模型.
  • 探索电子进化与摩擦能耗之间的关系.

主要方法:

  • 使用密度函数理论 (DFT) 的计算.
  • 分析沿着滑动路径的电子密度变化
  • 在滑动过程中跟踪摩擦能耗.

主要成果:

  • 表面摩擦与阻碍接触配置变化的电子屏障有关.
  • 摩擦能耗表现出对电子演变的线性依赖.
  • 电荷演变模型将摩擦与电子重新排列相关联.
  • 该模型提供了切割强度和真实接触面积假设的见解.

结论:

  • 电子相互作用基本上控制了各种键类型 (范德瓦尔斯键,金属键,离子键,共价键) 的界面摩擦.
  • 电荷演变模型为电子层面的摩擦提供了新的视角.
  • 这项工作为设计纳米机械设备和理解自然故障机制铺平了道路.