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相关概念视频

Metallic Solids02:37

Metallic Solids

16.4K
Metallic solids such as crystals of copper, aluminum, and iron are formed by metal atoms. The structure of metallic crystals is often described as a uniform distribution of atomic nuclei within a “sea” of delocalized electrons. The atoms within such a metallic solid are held together by a unique force known as metallic bonding that gives rise to many useful and varied bulk properties.
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and...
16.4K
Poisson's And Laplace's Equation01:25

Poisson's And Laplace's Equation

4.3K
The electric potential of the system can be calculated by relating it to the electric charge densities that give rise to the electric potential. The differential form of Gauss's law expresses the electric field's divergence in terms of the electric charge density.
4.3K
Electrostatic Boundary Conditions01:16

Electrostatic Boundary Conditions

1.2K
Consider an external electric field propagating through a homogeneous medium. When the electric field crosses the surface boundary of the medium, it undergoes a discontinuity. The electric field can be resolved into normal and tangential components. The amount by which the field changes at any boundary is given by the difference between the field components above and below the surface boundary.
The surface integral of an electric field is given by Gauss's law in integral form and is related to...
1.2K
Electrostatic Boundary Conditions in Dielectrics01:27

Electrostatic Boundary Conditions in Dielectrics

2.1K
When an electric field passes from one homogeneous medium to another, crossing the boundary between the two mediums imparts a discontinuity in the electric field. This results in electrostatic boundary conditions that depend on the type of mediums the field propagates through.
Consider a case where both the mediums across a boundary are two different dielectric materials. Recall that the electric field and electric displacement are proportional and related through the material's permittivity....
2.1K
Boundary Conditions for Current Density01:25

Boundary Conditions for Current Density

1.5K
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.
1.5K
Differential Form of Maxwell's Equations01:17

Differential Form of Maxwell's Equations

1.5K
James Clerk Maxwell (1831–1879) was one of the significant contributors to physics in the nineteenth century. He is probably best known for having combined existing knowledge of the laws of electricity and the laws of magnetism with his insights to form a complete overarching electromagnetic theory, represented by Maxwell's equations. The four basic laws of electricity and magnetism were discovered experimentally through the work of physicists such as Oersted, Coulomb, Gauss, and...
1.5K

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相关实验视频

Updated: Apr 29, 2026

Fabrication and Operation of a Nano-Optical Conveyor Belt
11:10

Fabrication and Operation of a Nano-Optical Conveyor Belt

Published on: August 26, 2015

11.2K

在 FDTD 中的分散型 VP-EP 符合网格算法,用于 CCPR 模型.

Yuan Fan, Yuhao Zhou, Yanan Liu

    Optics express
    |February 20, 2026
    PubMed
    概括

    一个新的算法,分散体积-平均极化有效允许度 (D-VP-EP),使复杂的3D材料的准确分析. 这种方法在先进的电磁模拟中显著减少了计算资源和网格错误.

    科学领域:

    • 计算电磁学的计算.
    • 材料科学是一种材料科学.

    背景情况:

    • 精确模拟分散材料对于先进的电磁应用至关重要.
    • 像有限差异时间域 (FDTD) 这样的现有方法与复杂的几何形状和材料分散性作斗争.
    • 符合性网格对分散性材料具有挑战性,导致错误.

    研究的目的:

    • 介绍一种新的算法,分散体积-平均极化有效允许度 (D-VP-EP),用于分析3D分散材料.
    • 为了使在FDTD框架内具有任意极的分散材料之间实现对应性网格.
    • 为了降低计算成本,提高电磁模拟的准确性.

    主要方法:

    • 在FDTD方法中使用复杂结合极余 (CCPR) 模型.
    • 采用频域匹配算法和空间域插值算法.
    • 为了兼容性,保持常规CCPR-FDTD的代配方.

    主要成果:

    • D-VP-EP算法成功地减少了曲线接口上的网格不匹配错误.
    • 通过显著减少计算资源 (1/16),实现了与现有方法可比的准确性.
    • 在纳米球的散射模拟和微环的传输频谱模拟中证明了有效性.

    结论:

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    • D-VP-EP算法提供了一个高效和准确的解决方案,用于模拟3D分散材料与符合性网格.
    • 它克服了传统方法的局限性,提供了大量的计算节省.
    • 这一进步对纳米光子设备和元材料的设计和分析有重大影响.