I was attempting to make a model of a .625 wavelength antenna that included a trombone style matching system as found on the I-10K and Shockwave antennas, and I succeeded, although it took me a while to get the model to tune properly.
The first image will show the layout and the current distribution of the antenna.
As we can see in this image we have a tapped trombone matching system. We also have two high current locations on the antenna, one is where we would expect it to be 1/4 wavelength down from the tip, and the other is in the matching system. This is to be expected on this type of antenna.
A note on the trombone matching system, there are a few limitations about using this system when it comes to modeling, I will discuss them below.
Next we see the radiation pattern.
The first thing to note here is, while close, the pattern is not the same on both sides, that is because the matching system is causing a slight skewing of the model. I would expect less skewing in the pattern of the actual antenna as the matching system as modeled I was unable to get to include the curve I mentioned above. There will still be some skew, but the skewing will be less, making the pattern more even than it is now.
Next we will look at the antenna data.
As we can see, the antenna tuned very well. With some playing I could get the tunign even better, but as it is, we are already better tuned than an SWR meter by itself would tune, we are also more accurate than most antenna analyzers will show, so I am happy with this.
The next thing to look at is the Efficiency and Rad-eff numbers. The Radiat-eff number is telling you how much of the total power going to the antenna is being radiated to the far field. The Efficiency number tells you how much of that power is being lost int eh antenna itself. In this case, all of that is from the antenna material I used, which is T6 Aluminum. 0.14% of the power is being lost to heat simply due to the material the antenna was made out of. This is also reflected in the Structure loss number in conjunction with the Input power number.
Next we see the SWR graph.
The middle half of these charts is the CB band. This should give an idea about bandwidth.
Also impedance (X and R).
And finally, for those who like smith charts, the range of frequencies in the above graphs as plotted on a smith chart. For those who are unfamiliar, everything within the black circle is under 2:1 SWR.
A few notes on this model.
1) The antenna's radials are about 1 wavelength above poor ground.
2) To get this antenna to where it could be tuned normally I had to use a smith chart to plot the frequency range used. Normally we tune antennas so X=0, but there was no X=0 point until I got the matching system close enough to a match. Once we got to a certain point, using X as a means for tuning wasn't a problem, but if you try and make such a model from scratch, you will likely have the same issue.
3a) One other note about this matching system that didn't come up. On the actual antennas, the bottom part of the trombone matching system is either in line with the radials, or immediately above them. Due to the limitations of the NEC2 engine, I was unable to put the matching system in line with said radials, or any lower above the radials. This is a limit that I have to live with working with the NEC2 engine.
3b) A side effect of 3a is if you look closely at the radials in the first image above, you will see that the currents on the two on the left are slightly stronger then the currents on the two on the right. This is due to the matching system layout, and if I were to get the matching system lower, like it is on the actual antennas, the difference in currents for the radials would be even larger. We could account for this to a point by making two of the radials slightly longer, but that is not how these antennas are sold.
4) While the antenna is made completely out of T6 aluminum, it is also entirely 6mm (about half an inch) in diameter. Parts of the actual antennas have different diameters. Because of this there will be a slight difference in various aspects of the antenna, but noting big.
The DB
The first image will show the layout and the current distribution of the antenna.
As we can see in this image we have a tapped trombone matching system. We also have two high current locations on the antenna, one is where we would expect it to be 1/4 wavelength down from the tip, and the other is in the matching system. This is to be expected on this type of antenna.
A note on the trombone matching system, there are a few limitations about using this system when it comes to modeling, I will discuss them below.
Next we see the radiation pattern.
The first thing to note here is, while close, the pattern is not the same on both sides, that is because the matching system is causing a slight skewing of the model. I would expect less skewing in the pattern of the actual antenna as the matching system as modeled I was unable to get to include the curve I mentioned above. There will still be some skew, but the skewing will be less, making the pattern more even than it is now.
Next we will look at the antenna data.
As we can see, the antenna tuned very well. With some playing I could get the tunign even better, but as it is, we are already better tuned than an SWR meter by itself would tune, we are also more accurate than most antenna analyzers will show, so I am happy with this.
The next thing to look at is the Efficiency and Rad-eff numbers. The Radiat-eff number is telling you how much of the total power going to the antenna is being radiated to the far field. The Efficiency number tells you how much of that power is being lost int eh antenna itself. In this case, all of that is from the antenna material I used, which is T6 Aluminum. 0.14% of the power is being lost to heat simply due to the material the antenna was made out of. This is also reflected in the Structure loss number in conjunction with the Input power number.
Next we see the SWR graph.
The middle half of these charts is the CB band. This should give an idea about bandwidth.
Also impedance (X and R).
And finally, for those who like smith charts, the range of frequencies in the above graphs as plotted on a smith chart. For those who are unfamiliar, everything within the black circle is under 2:1 SWR.
A few notes on this model.
1) The antenna's radials are about 1 wavelength above poor ground.
2) To get this antenna to where it could be tuned normally I had to use a smith chart to plot the frequency range used. Normally we tune antennas so X=0, but there was no X=0 point until I got the matching system close enough to a match. Once we got to a certain point, using X as a means for tuning wasn't a problem, but if you try and make such a model from scratch, you will likely have the same issue.
3a) One other note about this matching system that didn't come up. On the actual antennas, the bottom part of the trombone matching system is either in line with the radials, or immediately above them. Due to the limitations of the NEC2 engine, I was unable to put the matching system in line with said radials, or any lower above the radials. This is a limit that I have to live with working with the NEC2 engine.
3b) A side effect of 3a is if you look closely at the radials in the first image above, you will see that the currents on the two on the left are slightly stronger then the currents on the two on the right. This is due to the matching system layout, and if I were to get the matching system lower, like it is on the actual antennas, the difference in currents for the radials would be even larger. We could account for this to a point by making two of the radials slightly longer, but that is not how these antennas are sold.
4) While the antenna is made completely out of T6 aluminum, it is also entirely 6mm (about half an inch) in diameter. Parts of the actual antennas have different diameters. Because of this there will be a slight difference in various aspects of the antenna, but noting big.
The DB
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