I have often lamented that I have no antennas for the WARC bands: 30, 17 and 12 meters. Making or buying antennas for these bands is easy enough, it's just that I primarily focus on the HF contest bands and I don't want to crowd the towers and create unwanted interactions. I have relied for years on antennas that can be matched with a rig ATU (or the wide range of a manually-tuned tube amp), and kept pushing off better performing antennas for those bands.
I can get away with it since many of my antennas are high. Height can compensate for poor efficiency and pattern. I do pretty well in the DX pile ups on those bands. Nevertheless it is a gap in my station. In the heat of summer and while waiting for the hay to be harvested I decided to undertake construction of a simple 30 meter antenna.
Although it's simple, it is worth an article. The reason is that many of the mechanical and electrical issues I dealt with are commonly encountered by hams choosing, designing and building antennas. Hopefully this somewhat lengthy article will prove helpful to some readers.
I had several objectives for the antenna's design and deployment:
- DX friendly: I operate the WARC bands solely to chase DX. That means low elevation angles.
- Omni-directional: Directionality requires rotation or electrical direction switching, which is far more investment than I want for a simple antenna that will not see heavy use.
- Interaction: My contest band antennas have priority. I won't tolerate interactions (which are almost always detrimental) from this antenna.
- Support: The main towers are in a hay field. I need the antenna to be entirely off the ground, including supports, so that tractors can freely drive beneath it.
- Simplicity: I have enough maintenance challenges that I do not want this new antenna to create a lot of unwanted work in the future.
My choice was a vertically polarized delta loop, fed ¼ of the side length up from a bottom corner. This is a common method to achieve vertical polarization in a delta loop. Elevation angle is low, it's omni-directional, doesn't interact with horizontal yagis, and it's simple.
In this model, the delta loop is 1 meter from tower centre and the bottom is 5 meters high -- as built, the antenna is 0.7 meters from tower centre and 6 meters high. That places the apex at about 15 meters, about 8 meters below the lower 5-element yagi of the 20 meter stack. There is one guy threading the delta loop since the lowest guy station is at ~30' (9 m).
I modelled the tower as a long, thick vertical wire. As for shunt feeding the tower on 160 meters, I had to estimate the effective (electrical) height to approximate capacitance loading of the several yagis. I omitted the guys since they are broken into short non-resonant sections and likely have a small effect. Longer guy segments are located far from the tower and will not affect the delta loop even if there is near resonance at 10.1 MHz. I am more attentive to the effects for a directional antenna since the pattern nulls are easily perturbed.
The tower affects both pattern and resonance. It will still work if placed snug against the tower -- with suitable insulation since that's a high voltage node on the loop -- but will be detuned. If placed further outboard it can become difficult to install and maintain, and the pattern becomes more directional. I wrote about these parameters long long ago.
Rather than ask you to interpret those old words, here are a few notes to keep in mind:
- I used NEC5. Although accuracy is not critical for this antenna, the close spacing of the delta loop and tower is challenging for NEC2. There is no good way to align wire segments as NEC2 requires. Resonance dropped 500 kHz in NEC5 compared to NEC2. From my field measurements while building this antenna, NEC5 better reflects reality.
- The electrical height of the tower affects antenna resonance a small amount so it is not critical. Other factors dominate this antenna's behaviour.
- The closer the delta loop and tower the more omni-directional the pattern and the lower the resonant frequency. The first makes sense since with closer spacing the induced current will be closer in amplitude and phase.
- Why the strong coupling? Look at the current plot (above left). For a vertically polarized delta loop the voltage nodes (current nulls) are at the two points where the loop and tower are closest and therefore coupling greatest. This is a critical component of Moxon design, as one example. For a delta loop we need to be aware of the coupling if only because it affects antenna dimensions and demands good insulators at bottom centre and apex.
30 meters is only 50 kHz wide (0.5%) so it is easy to achieve a low SWR across the band, as the NEC2 model's SWR demonstrates. The matching network is a λ/4 transformer made from a 4.9 meter length of 75 Ω coax, included in the EZNEC model. The NEC2 unadjusted feed point impedance is about 115 Ω, which is typical for a full wave loop. The feed point is ¼ leg length (2.5 m) from a bottom corner. If you prefer a mix of vertical and horizontal radiation, a typical choice is to feed the antenna at a bottom corner. Expect a small impedance change, though not enough to justify a different matching network.
That's enough for now about the NEC2 model. Let's move onto construction before dealing with the model errors. Despite being a simple antenna there are several potential trouble points to be considered.
The bottom of the delta loop is made from aluminum tubing. This was done to meet the criterion of no ground anchors. I chose a couple of long tapered surplus yagi elements from my aluminum stock and spliced the inner 1" OD tubes with a 1.315" pipe. It's about 9.5 meters long -- the 3 sides add up to about 30 meters, or 1 wavelength).
Surplus #12 insulated wire from a decades-old wire antenna was used for the two sides. The EZNEC wires include the insulation since the lower velocity factor shortens the required length, typically 2% (VF of 0.98). As is typically recommended for wire antennas, I cut the wires a little long. They can be trimmed to bring the antenna into resonance where you want.
The sides of the loop pull up the drooping long bottom tubing and provide tension to the structure. The tower bracket keeps the bottom in position and prevents it from rotating in the wind (picture and description further below). The ABS pipe insulates the bracket from the antenna. A good insulator is needed since the centre of the bottom side is at a voltage node.
A vertically-polarized full-wave loop doesn't have to be high to work well. As you take it higher there is more radiation at higher elevation angles and that is usually (but not always!) less than ideal for DXing. However, ground loss increases at lower heights. There's a tradeoff.
I had to choose a height that minimized potential interaction with the 20 meter yagi up 23 meters while allowing clearance for farm machinery. My initial choice of 4.5 meters was increased to 6 meters to be certain of avoiding collisions. It is still well below the bottom 20 meter yagi.
The other interaction consideration is the cage gamma rod alongside the tower. The tower is shunt fed on 160 meters. There will likely be a tuning impact on 160 that I'll have to compensate for. Since the radials are removed for farming operations that can't be done yet.
I temporarily connected the delta loop to the 160 meter transmission line and made the required changes in my antenna selector software. By fall, when the 160 meter antenna is back in service, I'll add an auxiliary switch so that the antennas can share the transmission line. There is no foreseeable case where both antennas will be used at the same time.
I made brackets in my workshop for connecting the wire sides of the loop to the aluminum tubing bottom. Small strips of aluminum are held to the tube by hose clamps. There is a lip to keep the strips from slipping out. The wires are connected to the slanted upward end of the bracket by ¼" stainless bolt. Smaller bolts are strong enough but the smaller washers are insufficiently wide for wrapping #12 wire. The wire ends are looped and tinned for strength and to protect against corrosion, respectively.
The brackets can be slid along the tube for fine adjustment of antenna resonance without having to cut the wires. That feature came in useful.
The ¼λ transformer is made from RG59. It is found cheaply at local flea markets and is sufficient for the lower power permitted on 30 meters. It might handle a kilowatt but I don't intend to find out! The coax is coiled into a scramble wound CMC (common mode choke). It's less than ideal but good enough for a simple antenna like this one. Use a better choke if you prefer, but take into account its weight on the wire side of the loop.
When I modelled the antenna I added wires to simulate common mode on the outer side of the coax shield going down to the ground. To my surprise it had a deleterious impact on the pattern. Modelling the coax outer shield proved beneficial since even simple antennas can behave in ways you might not expect.
The RG59 solid centre conductor is fragile so I didn't want it swinging in the wind. Coiling the coax and binding it to the feed point insulator helps to avoid trouble. There is no wind induced flexing of either the open wire ends of the RG59 or the antenna wires. I added a short length of stranded and tinned wire to the centre conductor to further protect it should there be any unexpected movement. Weatherproofing of the open RG59 end was done after the picture was taken.
The LMR400 feed line is unsupported between the feed point and the tower. One advantage of LMR400 in this application is that it is lighter than many alternatives, included the heavier RG213. Their wind loads are equal and that may be a factor of coax choice if strong wind is a concern. RG58 might be a better choice for that case but, again, power handling might be an issue for bands other than 30 meters.
When the wire sides were draped over the tower guy station and connected to the bottom section, the bottom corners of the loop were slightly off the ground. This was my chance to do a "sanity" check. It may seem odd if you've never seen it done before, I connected the analyzer and swept the SWR over a wide range.
Obviously the antenna is nowhere near functional in this state! However, this test will indicate whether the antenna is functional. There will be excess ground loss and significantly lowered resonance since it is sitting on the ground, and the apex is draped over a conductor (the guy station anchor). The SWR dip down to about 4 at 8 MHz was a satisfactory result. Had there been no dip around that frequency I would have checked all the connections to see if there was a mistake. I've done the same test with tri-band yagis propped up a few feet above ground.
Confident that the antenna was approximately correct, I weatherproofed the exposed conductors and capped the coax connector. Raising the delta loop for a proper test was delayed a few days while I attended to other matters during a bout of extreme heat (well, for us). Working outdoors was unpleasant.
The apex of the raised delta loop is a convenient distance below the long tube that supports the top of the 160 meter gamma rod. So that became the upper support. Rather than tying the dacron rope directly to the wire, I routed the wire over a large thimble I pulled from my junk box. The thimble avoids a sharp bend in the wire and makes it easy to level the loop by sliding the wire over it. Since I was working alone I did it by observing the antenna's shadow.
Under tension the friction is high enough that the insulated wire is unlikely to shift. But it wouldn't be a bad idea to connect the wires on both sides of the thimble to limit motion. Don't pinch the wire since that can alter the tuning. Instead use a length of PVC or other plastic rod. Make it longer and the interior angle can be raised from 45° to the ideal 60°. The acute angle is due to wire sag. I can't increase wire tension any further since that pulls up the ends of the tube bottom side.
The support rope is looped over the gamma rod support tube several times. Tension and friction prevent the rope creeping along the tube. The rope is loosely tied to the tower to prevent it blowing in the wind. It is not a truss for the tube, as it may appear in the picture; the tube is strong enough on its own.
This is a view from the ground of the bottom side bracket. The hardware store utility angle is not strong enough for this application but it was handy and didn't require that I do any drilling. There is very little weight on the bracket since the apex support rope takes much of the strain. However, the wind load on a 10 meter long tapered tube is a danger. The ropes on either side of the ABS pipe provide lateral support.
If the antenna works well I'll replace the bracket with a stronger one. There is no rush.
When I tested the antenna in its final configuration it resonated at 9 MHz. That's more than 10% low! After further tests and modelling using NEC5 (as discussed earlier) I lopped 1 meter off each of the two sides -- shortening the loop by 7%. That's less than 10% but it is better not to overshoot when trimming wires. With several factors that influence resonance there is more than one way to reaching the desired endpoint.
Trimming raised the resonant frequency to 9.7 MHz, which is indeed about 7%. For the final adjustment I slid the wire brackets at the ends of the bottom tubes inward by 65 cm. That put the SWR curve where I wanted it.
The SWR is unfortunately difficult to read in the adjacent picture. The centre of the display is 10.1 MHz. The SWR is about 1.8 mid-band. I took the measurement with a 50' roll of LMR400 that was looped over my shoulder. The open run to the feed point drooped more than was ideal.
The SWR improved when the cable was properly dressed and routed down the tower face. However it was still no better than 1.5. When I returned to EZNEC I discovered the reason. I had neglected to rerun the SWR plot using NEC5. NEC2 did not correctly calculate the impedance due to close coupling to the tower.
The tight coupling lowered the feed point impedance to between 75 and 80 Ω. That is much lower than the 115 Ω calculated by NEC2. The RG59 ¼λ transformer is doing nothing at all since its nominal impedance is the same as the antenna. I could do away with it but it's still handy as a common mode choke.
The insects and heat were insane so I decided that this was close enough. The rig put power into the antenna just fine without the ATU.
That's the completed antenna. There is enough tension in the support rope to pull up the ends of the bottom side a small amount. That adds stability to the antenna. Also notice that the coax is routed so that it comes off the side at close to a right angle to reduce coupling. It can't be entirely eliminated since the coax must traverse the interior of the loop when fed for vertical polarization. The 3 sides are not quite equal but close enough not to noticably impact performance.
That evening I put the antenna on the air. It was easy to be heard by the DX stations I called on CW. However there weren't many DX stations on CW. I monitored FT8 and the antenna at least heard well, copying many stations in Asia. But I didn't transmit.
I will have to move the transmission line back to the 160 meter antenna since I need it for a couple of upcoming contests, despite the lack of radials. I hope to have the transmission line remotely switched for both antennas by September when I'll install the 160 meter radials in preparation for winter.