| -UnixWebMath- |
|
||||||||||||||||||||
| This script was developed at the Center for Computational Electromagnetics (CCEM) - University of Illinois at Urbana with funding from the Sloan Center for Asynchronous Learning Environments(SCALE) |
| WinWebMath -- | ||
|
Your job has been sucessfully submitted and is underway.
When it is completed it will be added to the completed jobs list: | ||
|
|
| This page will continue to load until your job is complete,feel free to stop loading at any time. |
| This script was developed at the Center for ComputationalElectromagnetics (CCEM) - University of Illinois at Urbana with fundingfrom the Sloan Center for Asynchronous Learning Environments (SCALE) | ||
| -UnixWebMath- |
In[1] :=
frequency=300.;
lgth=.80;
angle=80.5;
wirad=0.1;
<< notebooks/vdipole/fort.m;
<< notebooks/PatPlot.m;
{zin,dir,vdipole}=AnalyzeVDipole[frequency,lgth,angle,wirad];
Print["Input Impedance (Re, Im): ",zin];
Print["Directivity: ", dir];
PatPlot2DAll[vdipole];
PatPlot3D[vdipole, PlotPoints -> 60];
|
Mathematica Output |
Input Impedance (Re, Im): {148.2734, 272.5063}
Directivity: 3.12395
| Processed by Mathematica version 2.2 running on a UNIX platform. |
| This script was developed at the Center for Computational Electromagnetics (CCEM) - University of Illinois at Urbana with funding from the Sloan Center for Asynchronous Learning Environments(SCALE) |
The method of moments is one of the most widely used techniques for analyzing radiation problems. The following series of examples show how Mathematica and WebMath can be effectively used as an interface for codes based on that method.
The following simulation is done by a wire antenna MoM code running in conjuction with a simple transmission line code. Together these programs can perform the full-wave analysis of log-periodic dipole and monopole arrays operating in free-space. The ouput is then interpreted by Mathematica and displayed in a illustrative format.
| -UnixWebMath- |
|
||||||||||||||||||||
|
Mathematica Output |
Magnitude bar for relative admittance matrix contours:
Contour Plot of Admittance matrix for the Radiating elements(without feeder):
Elemental Impedances (real part, smallest element to largest element): Element 1 -> 2.94364 - 1657.64 I Ohms Element 2 -> 3.91626 - 1375.27 I Ohms Element 3 -> 5.59608 - 1131.71 I Ohms Element 4 -> 7.89697 - 917.689 I Ohms Element 5 -> 11.1576 - 723.907 I Ohms Element 6 -> 16.0757 - 551.064 I Ohms Element 7 -> 23.534 - 388.474 I Ohms Element 8 -> 36.1247 - 231.888 I Ohms Element 9 -> 59.1635 - 68.954 I Ohms Element 10 -> 100.904 + 121.111 I Ohms VSWR = 1.5398 For provided Zs. Real[Zin] = 42.71687 - 18.7385 I
| Processed by Mathematica version 2.2 running on a UNIX platform. |
| This script was developed at the Center for Computational Electromagnetics (CCEM) - University of Illinois at Urbana with funding from the Sloan Center for Asynchronous Learning Environments(SCALE) |