Yagi-Uda (YagiUda2p4.sdf)

Problem description

A Yagi-Uda array is a directional antenna consisting of several parallel dipole elements. Only one of these dipole elements is driven, the other elements being parasitic . Directionality is achieved by requiring that there be one longer element adjacent to the source element, which is referred to as the reflector. The rest of the elements being adjacent to the source but opposite to the reflector, and shorter than the source element, are referred to as directors. Yagi antennas are ubiquitous, and as such optimal parameters for dipole lengths and separations have been established. We go with values one would typically find in any text covering the matter. This example illustrates how to obtain the far field radiation pattern of a Yagi-Uda array.

This simulation can be performed with a VSimEM license.

Opening the Simulation

The Yagi-Uda example is accessed from within VSimComposer by the following actions:

• Select the New → From Example… menu item in the File menu.
• In the resulting Examples window expand the VSim for Electromagnetics option.
• Expand the Antennas option.
• Select 2.4 GHz Yagi Uda Antenna and press the Choose button.
• In the resulting dialog, create a New Folder if desired, and press the Save button to create a copy of this example.

All of the properties and values that create the simulation are now available in the Setup Window as shown in Fig. 156. You can expand the tree elements and navigate through the various properties, making any changes you desire. The right pane shows a 3D view of the geometry, if any, as well as the grid, if actively shown. To show or hide the grid, expand the Grids element and select or deselect the box next to Grid.

Fig. 156 Setup Window for the Yagi-Uda example.

Simulation Properties

This file allows the modification of the antenna operating frequency, antenna dimensions, and simulation domain size.

By adjusting the dimensions any sized Yagi-Uda array can be simulated.

Running the Simulation

After performing the above actions, continue as follows:

• Proceed to the Run Window by pressing the Run button in the left column of buttons.
• Here you can set run parameters, including how many cores to run with.
• When you are finished setting run parameters, click on the Run button in the upper left corner of the Logs and Output Files pane. You will see the output of the run in the right pane. The run has completed when you see the output, “Engine completed successfully.” This is shown in Fig. 157.

Fig. 157 The Run Window at the end of execution.

Analyzing the Results

Proceed to the Analyze Window by pressing the Analyze button in the left column of buttons.

Select “computeFarFieldFromKirchhoffBox.py” from the analyzer list, and click “Open.”

The default parameters are sufficient for this problem. Input 10.0 for the farFieldRadius parameter and run the analyzer by clicking the “Analyze” button.

Visualizing the results

Proceed to the Visualize Window by pressing the Visualize button in the left column of buttons.

To view the near field pattern, do the following:

• Expand Scalar Data
• Expand E
• Select E_x
• Click Colors
• Check the Fix Minimum box and set the value to -0.1
• Check the Fix Maximum box and set the value to 0.1, then click “OK”
• Expand Geometries
• Select poly (YagiUda2p4PecShapes)
• Select Clip All Plots
• Move the dump slider forward in time

Fig. 159 The electric field near-field pattern.

The far field radiation pattern can be found in the scalar data variables of the data overview tab underneath the farE field. Check the farE_magnitude box, remove the minimum and maximum restrictions on colors, and uncheck Clip All Plots.

Fig. 160 The electric field manifestation of the far field pattern.

Further Experiments

Try adding more directors and changing their dimensions to see the effect on the far field pattern.