Python 3D electromagnetic FDTD simulator detailed tutorial: How to use PyTorch backend to optimize simulation on GPU

1 Introduction

With the continuous advancement of computing technology, various simulation technologies have attracted increasing attention. Among them, the 3D electromagnetic FDTD (finite difference time domain) simulator is a commonly used simulation method in the field of electromagnetics. Although there are many mature commercial software that support FDTD simulation, developing a simple simulator independently can better understand its working principle and adjust it according to specific needs.

This article will guide you in using Python to write a basic 3D electromagnetic FDTD simulator, and introduce how to use PyTorch's GPU acceleration function to improve simulation speed.

2. FDTD Basics

FDTD is a numerical method that solves Maxwell's equations directly in the time domain. By discretizing space and time, the continuous Maxwell equations are transformed into a series of discrete difference equations, and then the time evolution of the electric and magnetic fields is obtained through iteration.

The main equations are as follows:

  1. 更新磁场: Hxn+1/2=Hxn−Δt(∂Ezn∂y−∂Eyn∂z)H_x^{n+1/2} = H_x^n - \Delta t \left( \frac{\partial E_z^n}{\partial y} - \frac{\partial E_y^n}{\partial z} \right)Hxn+1/2​=Hxn​−Δt(∂y∂Ezn​​−∂z∂Eyn​​) Hyn+1/2=Hyn−Δt(∂Exn∂z−∂Ezn∂x)H_y^{n+1/2} = H_y^n - \Delta t \left( \frac{\partial E_x^n}{\partial z} - \frac{\partial E_z^n}{\partial x} \right)Hyn+1/2​=Hyn​−Δt(∂z∂Exn​​−∂x∂Ezn​​) Hzn+1/2=Hzn−Δt(∂Eyn∂x−∂Exn∂y)H_z^{n+1/2} = H_z^n - \Delta t \left( \fra

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Origin blog.csdn.net/qq_38334677/article/details/133084301