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fdtd100
- 简单的fdtd算法的matlab实现，能够模拟电源和高斯分布的面源-fdtd simple algorithm to achieve the Matlab to simulate power and Gaussian Surface
2D-FDTD-TM-RCS
- 这是一个用FDTD算法计算二维金属方柱散射场RCS的matlab程序.采用UPML吸收边界条件和高斯脉冲源激励,对于学习FDTD方法中的激励源加入,近-远场外推,吸收边界设置等很有帮助 -This is a two-dimensional metal with the FDTD algorithm to calculate the scattering RCS of a square cylinder matlab program. UPML absorbing boundary condi
TM_FDTD
- 二维TM波的FDTD算法，激励为高斯脉冲-Two-dimensional TM wave FDTD algorithm for the Gaussian pulse excitation
2D_TE_PML
- 空间上为高斯型的连续平面波入射到一薄金属层上的透射情况-Space for the continuous Gaussian plane wave incident on a thin metal layer on the transmission case
fdtdpml
- 本程序为一维fdtd代码。激励为高斯脉冲。边界为pml。-This program is one-dimensional fdtd code. Gaussian pulse excitation. Boundary pml.
2dpecgaussian
- 2d fdtd pec with gaussian source
myFDTD01
- FDTD Finite-Difference Time-domain free space no ABC FDTD(t) runs FDTD for time t. FDTD implements the FDTD/staggered leapfrog scheme over time 0-max_time and space 0-max_space. This program simulates a gaussian pulse in the grid specifi
Untitled13
- FDTD Finite-Difference Time-domain free space no ABC FDTD(t) runs FDTD for time t. FDTD implements the FDTD/staggered leapfrog scheme over time 0-max_time and space 0-max_space. This program simulates a gaussian pulse in the grid specifi
dipole_1
- This program is a very basic three-dimensonal FDTD program with a source in the middle of the problem space.This similar to the two dimensonal problem but here we assume that the source is not a point source. A simple Dipole Antenna consists of tw
fd1d_1.2
- 一维情况下用ＦＤＴＤ方法模拟电磁波的传播情况，加了吸收边界条件，用Ｃ和MATLAB混合编程，信号源是高斯脉冲-One-Dimensional FDTD simulation with the propagation of electromagnetic waves, plus the absorbing boundary condition, mixed with the C and MATLAB programming, the signal source is a Gaussian puls
fd2d_3.1
- 二维情况下用ＦＤＴＤ方法模拟电磁波的传播情况，没加吸收边界条件，用Ｃ和MATLAB混合编程，信号源是高斯脉冲-Two-dimensional case with the FDTD simulation of electromagnetic wave propagation, no additional absorbing boundary condition, mixed with the C and MATLAB programming, the signal source is a Gaus
fd2d_3.2
- 二维情况下用ＦＤＴＤ方法模拟电磁波的传播情况，加入了理想匹配层，用Ｃ和MATLAB混合编程，信号源是高斯脉冲-Two-dimensional case with the FDTD simulation of electromagnetic wave propagation, no additional absorbing boundary condition, mixed with the C and MATLAB programming, the signal source is a Gaus
FTDT2D
- 一个二维的FDTD程序 matlab程序 中间加高斯脉冲源 PML-A two-dimensional FDTD program matlab program the middle of the Gaussian pulse source PML
fdtd_twomedium
- 采用fdtd方法，分别计算平面波照射到1维层介质的反射与透射以及在理想介质中的传播，场源可为高斯源或者正弦源，可以直观理解趋肤深度和边界概念-By fdtd method, were calculated to 1-dimensional plane wave radiation reflection and transmission media layer and spread in an ideal medium, the field for the Gaussian source or s
fdtd2dmur
- MATLAB program with FDTD simulating a gaussian wave incident in the cylinder using absourbing condiction MUR.
1d_fdtd-gaus-with-pec
- 一维线性高斯电流源时域有限差分算法，pec边界-One-dimensional linear Gaussian current source FDTD algorithm, pec boundary
FDTDzhalan
- 激励源为高斯脉冲波形的二维 平行板FDTD（时域有限差分）TM波仿真-Excitation source for the two-dimensional Gaussian pulse waveform parallel plate FDTD (Finite Difference Time Domain) TM wave simulation
FDTD-2d-without-pml
- fdtd_2d basic algorithum version 1 isotopic linear non-dispersive material an soft gaussian source Dirichlet boundary conditions grid size and time size is designated directly Ez mode electic field nomalized- fdtd_2d basic algori
FDTD-Drude-model
- isotopic linear non-dispersive material grid size and time size is designated directly electic field nomalized PML for all three directions fdtd 3d with drude model TF/SF wave analysis incorperating electric conductivity and mag
fdtd2
- 带挡板的二维平行板传输线FDTD仿真，使用高斯激励(FDTD Simulation of Gaussian Excited 2D Parallel Plate Transmission Line)