Description: TOYFDTD1 is a stripped-down minimalist, 3D FDTD code demonstrating the basic tasks in implementing a simple 3D FDTD simulation. An idealized rectangular waveguide is modeled by treating the interior of the mesh as free space and enforcing PEC conditions on the faces of the mesh. A simplified plane wave source is inserted at one end. First released 12 April 1999. Version 1.03 released 2 December 1999. Platform: |
Size: 34106 |
Author:蒋长宏 |
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Description: This a very simple Yee algorithm 3D FDTD code in C implementing the free space form of Maxwell s equations on a Cartesian grid. There are no internal materials or geometry. The code as delivered simulates an idealized rectangular waveguide by treating the interior of the mesh as free space/air and enforcing PEC (Perfect Electric Conductor) conditions on the faces of the mesh.-This a very simple algorithm 3D Yee FDTD code in C implementing the free space form of Maxwell's equations s on a Cartesian grid. There are no materials or internal geometry. The code as delivered simulates an idealized rectangular effort at by treating the interior of the mesh as free space / air and enforcing PEC (Perfect Electric Conductor) conditions on the faces of the mesh. Platform: |
Size: 9201 |
Author:吴婷 |
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Description: TOYFDTD1 is a stripped-down minimalist, 3D FDTD code demonstrating the basic tasks in implementing a simple 3D FDTD simulation. An idealized rectangular waveguide is modeled by treating the interior of the mesh as free space and enforcing PEC conditions on the faces of the mesh. A simplified plane wave source is inserted at one end. First released 12 April 1999. Version 1.03 released 2 December 1999. Platform: |
Size: 33792 |
Author:蒋长宏 |
Hits:
Description: This a very simple Yee algorithm 3D FDTD code in C implementing the free space form of Maxwell s equations on a Cartesian grid. There are no internal materials or geometry. The code as delivered simulates an idealized rectangular waveguide by treating the interior of the mesh as free space/air and enforcing PEC (Perfect Electric Conductor) conditions on the faces of the mesh.-This a very simple algorithm 3D Yee FDTD code in C implementing the free space form of Maxwell's equations s on a Cartesian grid. There are no materials or internal geometry. The code as delivered simulates an idealized rectangular effort at by treating the interior of the mesh as free space/air and enforcing PEC (Perfect Electric Conductor) conditions on the faces of the mesh. Platform: |
Size: 9216 |
Author:吴婷 |
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Description: 程序计算了国产矩形波导BJ-100的传输特性。通过查阅资料可以知道BJ-100波导管的结构参数为频率范围（8.2GHz~12.5GHz）结构参数a=22.86mm,b=10.16mm
FDTD计算 fortran 语言-Procedure to calculate domestic BJ-100 rectangular waveguide transmission characteristics. Through access to information can be aware of BJ-100 waveguide structural parameters for the frequency range (8.2GHz ~ 12.5GHz) structural parameters of a = 22.86mm, b = 10.16mm FDTD calculation fortran language Platform: |
Size: 7279616 |
Author:zhangmei |
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Description: FDTD（时域有限差分法）写的一个双脊金属加载矩形波导，的基模和第一个高阶模的色散曲线计算。-FDTD (finite difference time domain method) to write a双脊metal loaded rectangular waveguide, the fundamental mode and first higher order mode dispersion curve. Platform: |
Size: 2048 |
Author:李涛 |
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Description: 3维FDTD的MATLAB源程序，以充满空气的矩形腔共鸣器为例。-3-D FDTD the MATLAB source code to the air filled rectangular cavity resonator as an example. Platform: |
Size: 2048 |
Author:李彩云 |
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Description: 用FDTD法计算了填充各向异性介质的矩形波导的截止波数-It caculate the cut-off wavenumbers of rectangular waveguide which is filled with anisotropic medium Platform: |
Size: 2048 |
Author:王建敏 |
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Description: 用MATLAB编写的，基于时域有限差分算法求解矩形波导的TE模式场分布。-Written using MATLAB based FDTD algorithm for solving rectangular waveguide TE mode field distribution. Platform: |
Size: 1024 |
Author: |
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Description: 采用FDTD算法仿真矩型脊波导TM模色散曲线-The finite difference time domain Maxwell equations in the field of time and space differencing. Leapfrog space in the field of electric and magnetic fields alternate calculation, updated by the time field to mimic the changes in the electromagnetic field, to achieve the purpose of numerical calculation. The analysis of the problem to consider the geometric parameters of the object of study, the material parameters, calculation accuracy, computational complexity, computational stability and many other issues. The advantage is the ability to direct simulation of field distribution, the accuracy is relatively high, and is currently one of the more numerical simulation method.This course designe using the finite difference method combined with double-ridged rectangular waveguide boundary conditions to solve the fundamental mode of the waveguide and the first higher order mode dispersion curve. Platform: |
Size: 2048 |
Author:梁家军 |
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