80 Meter Wire LPDA's
For many years, the ARRL Antenna Book has contained an LPDA for 80 meters that uses 4 elements and is arranged as both a forward-sloping Vee and an inverted Vee, with its ends close to the ground. It was carefully designed from basic LPDA design equations with a Tau of 0.845 and a Sigma of 0.06, resulting in a #14 copper wire array close to 50′ from front to rear (ignoring the forward Vee extension).
Unfortunately, this array has a number of properties that reduce its potential performance:
- 1. The elements are Vee’d forward, reducing gain and decreasing the front-to-side ratio.
- 2. The elements are modified inverted Vees, again reducing gain and decreasing the front-to-side ratio.
- 3. The array uses thin wire, reducing gain relative to elements of an optimal diameter.
- 4. The combination of Tau (0.845) and Sigma (0.06) alone yield a maximum free-space gain potential to well under 6 dBi.
The combination of performance-degrading factors in this array strongly suggest that a redesign is in order. In these notes, I shall explore more adequate arrays for 80 meters. However, each will presume standard linear elements at right angles to the main array axis. In the course of these notes, we shall look at the question of optimal element size and how to simulate it with a wire array. We shall also examine some limits (and the reasons for those limits) of improving thin wire lower HF arrays with simulated fatter elements.
An Improved 6-Element Wire LPDA for 80 Meters
Figure 1 shows the outline of an LPDA using 6 elements, with a Tau of 0.8918 and a Sigma of 0.0702. The Tau and Sigma values are the initial values of the design. However, the element lengths have been optimized for the best performance across the 80-meter band (3.5-4.0 MHz) using standard circularized-Tau techniques. The final design–which might still be improved further with judicious experimentation–retains the original spacing, but 4 of the 6 elements have modified lengths.
Key to array performance is the element diameter, specified in the original design as 2″. The elements are modeled as copper, although there is less than 0.02 dB difference between copper and aluminum when the elements are as fat as specified here.
The following table provides the wire specifications in the form of a NEC wire table. The phase line has a characteristic impedance of 100 Ohms.
3.3-4.5 MHz t=.89 s=.07 Frequency = 4 MHz.
Wire Loss: Copper — Resistivity = 1.74E-08 ohm-m, Rel. Perm. = 1
Wires
Wires | End 1 X (feet) | End 1 Y (feet) | End 1 Z (feet) | End 2 X (feet) | End 2 Y (feet) | End 2 Z (feet) | Diameter (inches) | Segments |
---|---|---|---|---|---|---|---|---|
1 | 0.000 | -76.000 | 0.000 | 0.000 | 76.000 | 0.000 | 2.00E+00 | 91 |
2 | 21.346 | -67.800 | 0.000 | 21.346 | 67.800 | 0.000 | 2.00E+00 | 81 |
3 | 40.382 | -60.500 | 0.000 | 40.382 | 60.500 | 0.000 | 2.00E+00 | 73 |
4 | 57.358 | -55.500 | 0.000 | 57.358 | 55.500 | 0.000 | 2.00E+00 | 65 |
5 | 72.498 | -51.000 | 0.000 | 72.498 | 51.000 | 0.000 | 2.00E+00 | 59 |
6 | 86.000 | -47.500 | 0.000 | 86.000 | 47.500 | 0.000 | 2.00E+00 | 53 |
Sources
Source | Wire Segments | Wire # | Pct Actual | From End 1 | Specified | Ampl.(V, A) | Phase(Deg.) | Type |
---|---|---|---|---|---|---|---|---|
1 | 27 | 6 | 50.00 | 6 | 50.00 | 0.707 | 0.000 | V |
The performance of this array is quite good for an 86′ long LPDA on 80 meters, with an average free-space gain of about 6.9 dBi across the band. Whether the performance can be maintained in practice depends, of course, on the ability of the builder to raise the antenna to a height where horizontally polarized antennas perform well over desired propagation paths. The front-to-back ratio is above 20 dB across the band.
The use of 2″ diameter elements on 80 meters is exceptionally rare, given the need for elements that are at their longest 152′. As an experiment, I took the same array and tested it in model form using #12 AWG wire (0.0808″ diameter). Interestingly, the average free-space gain dropped to about 5.9 dBi with an average front-to-back ratio of about 13.5 dB. The loss of a full dB of gain in the move from 2″ to 0.0808″ element diameters seemed less than desirable.
Therefore, I reconstructed the elements from 2 parallel wires in accord with the sketch in Figure 2.
The principle, as I have elsewhere noted, consists in taking a representative element in the array and finding its self-resonant frequency. Then, I constructed a model of a two-wire element of the same length and varied the spacing between the wires until it was resonant at the same frequency. In the present exercise, a spacing of between 10 and 12 inches proved to be close to precise, with a remnant reactance of under 10 Ohms at the widest spacing used.
For modeling simplicity, I used the 12″ spacing, which translates into 1 foot (or a shortest segment length of 0.5′). See Figure 3.
Figure 3 shows the element model. The center portion is (for this model) 1.5′ long and consists of 3 segments to ensure that the source segment is equal in length to the segments adjacent to it. The single wire is also necessary within the LPDA array, since the phase-line must meet a single wire segment at each element in the array. On each side of center, single segment wires, each 0.5′ long, connect the center wire to the parallel wires that constitute the bulk of the elements. These wires, which have the same number of segments to sustain parallel segment junctions throughout, are connected together at the outer ends with 2-segment wires. The 11-wire element constitutes a reasonably fair model of the 2-wire element.
The attention to segment lengths at the center-most part of the element allowed me to reduce the number of segments in the long wires. Ideally, the segment length should be 0.5′ throughout the model, which would have resulted in about 150 segments per long wire in the longest element. However, reducing the number to about 50 yielded a change of reactance in the test element of under 5 Ohms. So reduced segmentation–but still with parallel segment junctions–was used in the final array model. For reference, the following partial table shows just 2 elements of the modified array.
80, t=.89 s=.07 Frequency = 3.5 MHz.
Wire Loss: Copper — Resistivity = 1.74E-08 ohm-m, Rel. Perm. = 1
Wires
Wire | Connection | End 1 X (feet) | End 1 Y (feet) | End 1 Z (feet) | Connection | End 2 X (feet) | End 2 Y (feet) | End 2 Z (feet) | Diameter (inches) | Segments |
---|---|---|---|---|---|---|---|---|---|---|
1 | W2E1 | 0.000 | -76.000 | -0.500 | W3E1 | 0.000 | -76.000 | 0.500 | 12 | 2 |
2 | W1E1 | 0.000 | -76.000 | -0.500 | W4E1 | 0.000 | -0.750 | -0.500 | 12 | 51 |
3 | W1E2 | 0.000 | -76.000 | 0.500 | W5E1 | 0.000 | -0.750 | 0.500 | 12 | 51 |
4 | W2E2 | 0.000 | -0.750 | -0.500 | W5E2 | 0.000 | -0.750 | 0.000 | 12 | 1 |
5 | W3E2 | 0.000 | -0.750 | 0.500 | W6E1 | 0.000 | -0.750 | 0.000 | 12 | 1 |
6 | W4E2 | 0.000 | -0.750 | 0.000 | W7E1 | 0.000 | 0.750 | 0.000 | 12 | 3 |
7 | W8E1 | 0.000 | 0.750 | 0.000 | W9E1 | 0.000 | 0.750 | -0.500 | 12 | 1 |
8 | W6E2 | 0.000 | 0.750 | -0.500 | W10E1 | 0.000 | 0.750 | 0.500 | 12 | 1 |
9 | W7E2 | 0.000 | 0.750 | 0.500 | W11E1 | 0.000 | 76.000 | -0.500 | 12 | 51 |
10 | W8E2 | 0.000 | 0.750 | -0.500 | W11E2 | 0.000 | 76.000 | 0.500 | 12 | 51 |
11 | W9E2 | 0.000 | 76.000 | -0.500 | W10E2 | 0.000 | 76.000 | 0.500 | 12 | 2 |
12 | W13E1 | 21.346 | -67.800 | -0.500 | W14E1 | 21.346 | -67.800 | 0.500 | 12 | 2 |
13 | W12E1 | 21.346 | -67.800 | 0.500 | W15E1 | 21.346 | -0.750 | -0.500 | 12 | 46 |
14 | W12E2 | 21.346 | -67.800 | -0.500 | W16E1 | 21.346 | -0.750 | 0.500 | 12 | 46 |
15 | W13E2 | 21.346 | -0.750 | 0.500 | W16E2 | 21.346 | -0.750 | 0.000 | 12 | 1 |
16 | W14E2 | 21.346 | -0.750 | 0.000 | W17E1 | 21.346 | -0.750 | 0.000 | 12 | 1 |
17 | W15E2 | 21.346 | -0.750 | 0.000 | W18E1 | 21.346 | 0.750 | 0.000 | 12 | 3 |
18 | W19E1 | 21.346 | 0.750 | 0.000 | W20E1 | 21.346 | 0.750 | -0.500 | 12 | 1 |
19 | W17E2 | 21.346 | 0.750 | 0.000 | W21E1 | 21.346 | 0.750 | 0.500 | 12 | 1 |
20 | W18E2 | 21.346 | 0.750 | -0.500 | W22E1 | 21.346 | 67.800 | -0.500 | 12 | 46 |
21 | W19E2 | 21.346 | 0.750 | 0.500 | W22E2 | 21.346 | 67.800 | 0.500 | 12 | 46 |
22 | W20E2 | 21.346 | 67.800 | -0.500 | W21E2 | 21.346 | 67.800 | 0.500 | 12 | 2 |
The use of the twin-wire (#12 AWG) elements restored much of the performance to the array–on average about 80% of the performance lost in going from a 2″ element to a #12 single wire element. The average free-space gain rose to over 6.6 dBi, with an average front-to-back ratio of over 20 dB.
However, a better measure of appreciating how well the double-wire elements simulate the tubular elements can be gleaned from some graphs.
Figure 4 shows the free-space gain across 80 meters a 0.05 MHz intervals. Not only is the double-wire curve much higher on average than the single wire curve, as well, it parallels the 2″ element curve very closely. The single-wire curve peaks at a quite different frequency to the peak for the upper two curves.
In Figure 5, for the front-to-back ratio, we find a similar pattern, with the 2″ element and the double-wire curves not only higher, but also more parallel than the curves for the single thin-wire version of the antenna.
Perhaps the least significant set of differences can be found in the 50-Ohm VSWR curve for the three versions of the array. shown if Figure 6. All would be acceptable 80-meter SWR curves. I shall note in passing that these curves are easy to obtain with experimental modeling shifts in the phase-line characteristic impedance. However, the original design equations called for a phase-line impedance of closer to 200 Ohms, with the illusion of needing a matching device for a coaxial feedline for the array.
The ability of a simple 2-wire element to restore most of the performance to the array arises from the fact that an LPDA–like any multi-element array–derives its performance not only from driving the elements, but as well from the mutual coupling between elements. The simulated fat elements, composed of wide-spaced wires, indeed has close to the same mutual coupling between array elements as the fat-wire model.
What differs between the 2-wire model and the fatter single-element version is the overall efficiency of the antenna. With 2″ elements, the array is about 99.7% efficient, with losses due to material resistance that are a small fraction of 1%. The single #12 wire version is about 95.9% efficient, with over 4% material losses. The double-wire version reaches an efficiency of about 97.1%, which is only about a third of the way above the efficiency of the single-wire version toward the fat-element version. In short, the double-wire version of the antenna cannot restore all of the performance of the fat-wire version because it cannot decrease wire losses to the level of a single fat element. However, it can restore a large portion of the mutual coupling lost by using a single then wire for each element.
The process of restoring performance has a limit, and another LPDA design can illustrate this limit.
A 14-Element Wire LPDA for 80 Meters
By judiciously changing the values of Tau and Sigma, it is possible to arrive at an LPDA design with even better performance than we have so far attained. Fig. 7 shows the outline of a 14-element 88.5′ long array, again, initially using 2″ elements.
The new array uses a Tau of 0.96 and a Sigma of 0.03 to pack the large number of elements into the prescribed space. Again, the phase-line characteristic impedance is 100 Ohms to arrive at a 50-Ohm feedpoint impedance. The following table shows the dimensions.
80m t=.96 s=.03 Frequency = 4 MHz.
Wire Loss: Copper — Resistivity = 1.74E-08 ohm-m, Rel. Perm. = 1
Wires
Wires | End 1 X (feet) | End 1 Y (feet) | End 1 Z (feet) | End 2 X (feet) | End 2 Y (feet) | End 2 Z (feet) | Diameter (inches) | Segments |
---|---|---|---|---|---|---|---|---|
1 | 0.000 | 0.000 | 0.000 | 0.000 | 2.00E+00 | 25 | ||
2 | 8.603 | 0.000 | 8.603 | 0.000 | 2.00E+00 | 25 | ||
3 | 16.862 | 0.000 | 16.862 | 0.000 | 2.00E+00 | 23 | ||
4 | 24.790 | 0.000 | 24.790 | 0.000 | 2.00E+00 | 23 | ||
5 | 32.402 | 0.000 | 32.402 | 0.000 | 2.00E+00 | 21 | ||
6 | 39.709 | 0.000 | 39.709 | 0.000 | 2.00E+00 | 21 | ||
7 | 46.723 | 0.000 | 46.723 | 0.000 | 2.00E+00 | 19 | ||
8 | 53.457 | 0.000 | 53.457 | 0.000 | 2.00E+00 | 19 | ||
9 | 59.922 | 0.000 | 59.922 | 0.000 | 2.00E+00 | 19 | ||
10 | 66.128 | 0.000 | 66.128 | 0.000 | 2.00E+00 | 17 | ||
11 | 72.086 | 0.000 | 72.086 | 0.000 | 2.00E+00 | 17 | ||
12 | 77.805 | 0.000 | 77.805 | 0.000 | 2.00E+00 | 17 | ||
13 | 83.296 | 0.000 | 83.296 | 0.000 | 2.00E+00 | 15 | ||
14 | 88.567 | 0.000 | 88.567 | 0.000 | 2.00E+00 | 15 |
Sources
Source | Wire Segments | Wire # | Pct Actual | From End 1 | Specified | Ampl.(V, A) | Phase(Deg.) | Type |
---|---|---|---|---|---|---|---|---|
1 | 8 | 14 | 50.00 | 14 | 50.00 | 0.707 | 0.000 | V |
Like the smaller array, this design employs a measure of circularized Tau to obtain better performance than provided by the initial design taken from LPDA equations. The rear-most 2 and the forward-most 3 elements have been modified, and further refinement may be possible.
With 2″ elements, the array has an average free-space gain across 80 meters of nearly 7.6 dBi, with an average front-to-back ratio of about 20 dB. A single #12 wire version of the antenna achieves an average free-space gain of about 6.75 dBi, about 0.8 dB lower than the fat-element version. Interestingly, the single-wire version of the antenna has an average front-to-back ratio of about 25 dB, about 5 dB higher than that of the fat-element version.
The same techniques used with the smaller array were applied to the 14-element LPDA to produce a double wire version. The resulting array model had over 2300 segments, even using the reduced levels of segmentation in the long parallel sections of each double-wire element. The resulting array showed an average free-space gain of about 7.1 dBi, less than half way toward the fat-element version from the single-wire model. The average front-to-back ratio was about 21 dB, close to the value of the fat-element version.
Figure 8 shows the gain curves for the three models. The double-wire and fat-wire versions are very synchronous, while the single-wire model curve shows divergent frequencies for its peaks and valleys.
In Figure 9, we see much the same results. The fat-wire and double-wire curves are closely matched, while the single-wire takes a direction of its own–and at a higher average level of front-to-back ratio.
In keeping with the front-to-back curves, Figure 10 shows 50-Ohm VSWR curves that are very similar for the fat-wire and double wire models. In contrast, although still a very flat curve, the single-wire SWR curve shows a progression of its own.
Initially, one might have expected a relatively uniform performance upgrade relative to that shown for the 6-element LPDA. However, 2 factors count against that expectation.
First, the efficiency of the larger array is inherently lower than that of the small LPDA. The fat-element version has an efficiency of about 99.2%, against a single #12 wire version efficiency of 88.5%. Doubling the wires for each element only raises the efficiency to 90.8%, a gain of 2.3% but still 8.4% shy of the fat wire model. From an efficiency perspective alone, the ability of the double-wire version to restore most of the performance of the fat-wire version is limited.
However, we should have also noted the fact that the LPDA front-to-back ratio decreased as we moved from the thin-wire to the fat-wire model. This fact suggests that the most closely spaced elements of the 14-element array are already over-coupled when using fat elements. Gain increases with wire size are largely functions of increased efficiency rather than superior mutual coupling between elements. The following table provides the key performance reports of NEC for the same 14-element array using a variety of element diameters ranging from the single-wire #12 AWG version up to and including the 2: element version. The progression may prove interesting for data taken at 3.75 Hz.
Element Diameter (inches) | Gain (dBi) | Front to Back Ratio (dB) | Feed Impedance R+/-jX Ohms | 50-Ohm VSWR |
---|---|---|---|---|
0.0808 | 6.80 | 26.25 | 62.9 – j 4.4 | 1.28 |
0.25 | 7.24 | 23.57 | 60.2 – j 6.9 | 1.25 |
0.5 | 7.37 | 21.91 | 55.0 – j 9.2 | 1.22 |
1.0 | 7.45 | 20.65 | 46.8 + j 8.2 | 1.20 |
1.5 | 7.48 | 20.03 | 42.3 – j 4.9 | 1.22 |
2.0 | 7.50 | 19.68 | 40.1 – j 1.5 | 1.25 |
The largest increment of gain occurs with the first move that increases the element diameter by a factor of 3. As well, the front-to-back ratio also shows its steepest decrease. Above that level, performance stabilizes within a quite narrow range.
The result for this particular model is a set of alternative building strategies. One might go to the trouble of constructing 14 sets of double-wire elements. However, one can get as much performance improvement of the single-thin-wire model by simply using 0.25″ wire, either copper or aluminum–the latter being lighter.
Conclusion
80-meter wire LPDAs can be effective horizontally polarized antennas for the entire band if they are better designed than past versions. Minimally, I would recommend the 6-element 86′ long model as an array whose effort at construction and mounting would be rewarded by decent performance. The double-wire version is apt for fixed installations, while–for certain builders with abilities matching the mass–the use of large tubular elements might well permit rotation of the antenna.
Further increments of performance will require larger arrays, such as the 14-element 88′ LPDA noted in the design exercise. However, because the elements have already reached the limits of their inter-element coupling, the double-wire version may be more work than is worth the effort. The use of a larger wire size–0.25″ or greater–may be the best way to improve performance above the level one can obtain from a single #12 wire.
Along the way, we have seen that the double-wire simulation of fat elements has a limit. The more elements to the array, the less the double-wire element can effectively restore performance lost when using single thin wires. Mutual coupling varies with several variables, including element spacing, element diameter, and frequency. The peaks and valleys evident in both gain and front-to-back curves for LPDAs arise largely because the mutual coupling among the most active elements does vary with frequency–variations in which also yield changes the current magnitude on each element in the array. The peaks and valleys in the performance curves are not coincident for both gain and the front-to-back ratio, suggesting that the optimal mutual coupling conditions for one parameter are not necessarily optimum for the other. However, since many elements are simultaneously active to a significant, if not controlling, degree, exacting formulations of the relationships lie beyond the realm of modeling. Nevertheless, in revealing the coincidence and displacement of curves as we vary the element diameter of the elements, modeling can show the effects of changes in coupling among elements.
The upshot of these exercises is this: it pays to explore a given design in many different kinds of models before deciding on the best method of construction.
Originally posted on the AntennaX Online Magazine by L. B. Cebik, W4RNL
Last Updated : 6th June 2024