基于物理信息的深度运营商网络用于模拟2D时域电磁波在各种媒体中的传播
Sooyoung Oh1, EungKyu Lee2, Sun K Hong1,3
1School of Electronic Engineering, Soongsil University, Sangdo-ro 369, Seoul 06978, South Korea.
iScience
|March 9, 2026
概括
基于物理学的深度运营者网络 (PI-DeepONet) 准确预测电磁波的传播. 与传统方法相比,这种方法为高频系统提供了更高的概括性,减少了重新培训的需要.
科学领域:
- 计算电磁学的计算.
- 应用物理学的应用物理学
- 机器学习是机器学习.
背景情况:
- 准确预测时间域电磁波 (EM) 对高频系统至关重要.
- 传统的有限差异时间域 (FDTD) 方法与大型计算领域相斗争.
- 基于物理学的神经网络 (PINNs) 提供了数据效率,但有限的概括性.
研究的目的:
- 开发一种更具通用性和高效的方法来建模二维瞬态电磁波传播.
- 研究物理知情深度操作员网络 (PI-DeepONet) 的应用,用于电磁波建模.
- 克服传统的解决方案和PINN在处理各种EM环境中的局限性.
主要方法:
- 将时间域赫尔姆霍尔茨方程纳入DeepONet架构.
- 开发了一个以物理为基础的深度运营商网络 (PI-DeepONet) 用于电磁波传播.
- 在各种激发和材料配置上训练PI-DeepONet模型.
主要成果:
- PI-DeepONet在不同来源位置和材料特性中展示了增强的概括性.
- 该模型成功地预测了自由空间和不均质介质中的波传播和散射.
- 空间时空电磁场的准确预测与FDTD模拟进行了验证.
结论:
- PI-DeepONet提供了一个强大而高效的替代模型,用于时间域EM分析.
- 该框架显示了在复杂环境中设计高频系统的巨大潜力.
- 这种方法增强了概括能力,减少了对模型再培训的需求.
更多相关视频
10:35Using Microwave and Macroscopic Samples of Dielectric Solids to Study the Photonic Properties of Disordered Photonic Bandgap Materials
Published on: September 26, 2014
12.8K
07:14Tracking Infiltration Front Depth Using Time-lapse Multi-offset Gathers Collected with Array Antenna Ground Penetrating Radar
Published on: May 1, 2018
8.2K
相关概念视频
Plane Electromagnetic Waves I
5.2K
The existence of combined electric and magnetic fields that propagate through space as electromagnetic (EM) waves is the most significant prediction of Maxwell's equations. As Maxwell's equations hold in free space, the predicted electromagnetic waves do not require a medium for their propagation. An EM wave comprises an electric field, defined as the force per charge on a stationary charge, and a magnetic field, which is the force per charge on a moving charge.
The EM field is assumed to be a...
The EM field is assumed to be a...
5.2K
Plane Electromagnetic Waves II
4.2K
Consider a plane wavefront traveling in position x-direction with a constant speed. This wavefront can be utilized to obtain the relationship between electric and magnetic fields with the help of Faraday's law.
4.2K
Propagation Speed of Electromagnetic Waves
4.8K
Electromagnetic waves are consistent with Ampere's law. Assuming there is no conduction current Ampere's law is given as:
4.8K
Electromagnetic Wave Equation
2.4K
Maxwell's equations for electromagnetic fields are related to source charges, either static or moving. These fields act on a test charge, whose trajectory can thus be determined using suitable boundary conditions. The objective of electromagnetism is thus theoretically complete.
However, although electric and magnetic fields were first introduced as mathematical constructs to simplify the description of mutual forces between charges, a natural question emerges from Maxwell's equations:...
However, although electric and magnetic fields were first introduced as mathematical constructs to simplify the description of mutual forces between charges, a natural question emerges from Maxwell's equations:...
2.4K
Electromagnetic Waves in Matter
4.1K
Electromagnetic waves can travel in the vacuum as well as in matter. For example light, which is an electromagnetic wave, can travel through air, water, or glass.
Consider the electromagnetic wave passing through a dielectric medium. In such a case, Maxwell's equations get modified. In Ampere's law, ε0 , the dielectric permittivity of free space is replaced with ε, the permittivity of dielectric. Also, the vacuum permeability μ0 is replaced by the permeability of the medium, μ.
Furthermore,...
Consider the electromagnetic wave passing through a dielectric medium. In such a case, Maxwell's equations get modified. In Ampere's law, ε0 , the dielectric permittivity of free space is replaced with ε, the permittivity of dielectric. Also, the vacuum permeability μ0 is replaced by the permeability of the medium, μ.
Furthermore,...
4.1K
Propagation of Waves
3.1K
When a wave propagates from one medium to another, part of it may get reflected in the first medium, and part of it may get transmitted to the second medium. In such a case, the interface of the two mediums can be considered as a boundary that is neither fixed nor free.
Consider a scenario where a wave propagates from a string of low linear mass density to a string of high linear mass density. In such a case, the reflected wave is out of phase with respect to the incident wave, however the...
Consider a scenario where a wave propagates from a string of low linear mass density to a string of high linear mass density. In such a case, the reflected wave is out of phase with respect to the incident wave, however the...
3.1K
