Along with location,
station equipment
and skills, aerials are one
of the most important
factors in DXing.
Main tower & 5 ele 15m
3 el tribander & 6m 3 el quad
Both towers seen from the North
Our hilltop rural QTH has space for two small towers for HF beams, and plenty of trees supporting LF wire antennas.
My 'main' tower is a steel lattice perched
on the highest point on the property,
and is about 12m high. The tiltover base
for this antenna is a large cube of
concrete. Currently there is a
15m 5 ele monoband yagi on it.
A second 12m tower, sited a few metres
lower, is supported on a heavy steel
telegraph pole keeper driven
into the subsoil with a digger >
Being a telescopic tiltover,
the lower tower is better
for testing and tweaking
antennas.
Both towers are guyed against the ferocious winds up here.
Although the beams are only about 12-14m off the ground, it helps enormously to be perched on top of a 260m hilltop from which the ground slopes steeply away all round.
The house is surrounded by macrocarpa trees planted about 100 years ago. At about 30m tall, the trees make good sky-hooks for my wire antennas - mostly fullwave loops and dipoles.
A 6m 3-element delta quad sort of worked
but I find much more magic
on the lower bands.
I hurriedly made and lashed-up a 160m
inverted-vee dipole to chase K5P
on Palmyra in 2016: it worked!
Temporary 160m inv-vee dipole
Second tower with experimental antennas
80m fullwave wire loop in the trees
Base of 30m vertical showing earth wire connecting the coax braid to the metal shed
Base of lower tower
LF loop in snow-covered trees
Simple wire antennas like dipoles and verticals are dead easy and very cheap to make: here’s how.
A sufficient length of suitable wire. Stranded wire is more flexible and resilient than single-core wire, in my experience, but some prefer hard-drawn copper. Plastic-coated wire reduces corrosion but increases the size and weight of the wire. Use my spreadsheets (below) to figure out how much you will need for, say a halfwave dipole or quarter wave vertical. There are tabs along the bottom for:
Antenna lengths in metres;
Antenna lengths in feet and inches
Stub lengths in meters, and in feet and inches
Antenna lengths in fathoms and other curious units of measure. Did you know the 10m band has a wavelength just short of the length of a London bus?
Explore on-screen
Download as PDF for printing
Metric version
Download as PDF for printing
Imperial version
A feedpoint insulator/connector, with a balun if you are feeding a balanced antenna with coax (e.g. a conventional dipole). There are several home-brew options here ranging from suitable pieces of wood, Perspex sheet, plastic or ceramic Tees or open-wire insulators, up to commercial centre pieces with built-in coax connectors. I make my own from IP56-sealed plastic boxes housing a ferrite toroid, using stainless steel bolts with stainless wing nuts for the antenna wires and either SO239 connectors or long coax pigtails terminated with in-line SO239s (again, to avoid unnecessary connectors and save the odd tenth of a dB - they all add up!). You should probably use ring terminal connectors of approximately 6mm to terminate and connect each leg of a dipole at the centre point, but soldered/tinned loops in the end of the wires will do. For unbalanced antennas such as wire verticals, simply solder the antenna wire and earth wires directly to the feeder centre and shield, respectively, then wrap the feed point with self-amalgam tape. “Chocolate block” screw-down electrical connectors can be useful when experimenting with new antenna designs or for field day lashups but don’t rely on them for permanent fixtures as they are hard to seal and corrode quickly.
Coax or open wire feeder, more than enough to reach from the antenna feedpoint once erected to the shack or remote antenna switch. Don’t go overboard but a few extra metres will allow for antenna movement in the wind and positioning the feeder to avoid garotting passing animals. Open wire feeder has negligible losses but the balun and ATU put the losses back in and add complexity, so open wire is only really worthwhile for a multiband doublet antenna, vee-beam or rhombic (dream on).
Antenna end insulators. Ceramic ones will last approximately forever (barring accidentally dropping them on the ground or over-stressing them) but are heavier and are quite scarce. Plastic ones will last up to a decade. Electric fence wire insulators are good if you have a farm supplies shop nearby, as they are designed to insulate tens of kilovolts for longterm outdoor use. Bits of Perspex or other strong plastic sheet can be cut to size. At a push, you may be lucky just using the plastic cord (see below) but it tends to start conducting when wet so the resonant point and match will change in the rain.
Self-amalgamating tape or coax sealant (NOT ordinary insulating tape - it won’t last more than a few days or weeks, although it does help protect the self-amalg from the sun’s UV).
A wooden winder board on which to wind the antenna. Make these from offcuts of plywood or thin MDF board approximately 30 x 15cm, with U-shaped notches in both short ends to hold the wire in place as you wind. Trust me, it’s quicker in the long run to make a bunch of these up and use them routinely than to untangle the wires and ropes/cords every time you go to erect a stored antenna.
Plastic cord to hoist the antenna. Fairly thin nylon or polypropylene cord is fine to hold out the ends of a small to medium-sized dipole or vertical, and lasts for ages if not over-stressed. Even nylon monofilament fishing line will do for small antennas, or maybe nylon strimmer line for larger ones. You will need thicker cord or rope (up to about 4-6mm) for large antennas and to hoist the balun and feeder of a dipole.
Measure out the exact wire lengths you will need and cut the wire. I usually do this by clamping the end of the wire plus the end of a long tape measure (another toolbox investment) in the workshop vice (there’s another!) and walking them out into the yard. If you have, say, a convenient fence or wall at least 10m long and some patience, you could measure and mark it permanently with paint or similar markers to use it as a giant ruler. Err on the long side as you will trim the antenna down to resonance later whereas adding wire would involve soldering-on extensions - more work and more weak points.
Make up the feed point, connecting the antenna wires via the balun to the feeder.
Seal the coax feed point with self-amalgam tape or coax sealant. Take care over this as any water entering the coax will ruin it forever.
Label the feedpoint with the band/type of antenna. Marker pen fades in a year or so but pencil lasts longer.
Erect the antenna and test it for resonance. Although it is more work, it is best to hoist it all the way up to its finished position. Assuming it is a bit LF of the desired resonance, bring the antenna down, trim a little off the ends, put it back up, re-test for resonance and repeat until done. If you get smart, calculating exactly how much you need to trim off, you will inevitably cut off too much at some point. As I said, err on the long side.
Work lots of DX!
There are several parameters to adjust when it comes to antennas but essentially the choices come down to gain (in both horizontal/azimuth and vertical/elevation planes, don’t forget) and pattern. I’ve had good DX results with vertical quarter-waves and inverted-vee dipoles, with reasonably low take-off angles and more-or-less omnidirectional in azimuth. I’ve never had tall enough towers at home to make horizontal antennas perform as per the textbooks (except in local contests where the high-angle radiation is useful) but even ground-mounted verticals seem to work well.
I suspend miscellaneous wire antennas in the trees from time to time. Loops seem to work better than verticals and dipoles, presumably due to their higher radiation resistance - around 125 ohms according to the books - and hence higher efficiency. Some experts claim they have lower angle radiation than dipoles but I’m not sure about that, and both factors presumably depend on their height above ground. They do seem to be low noise antennas, although that’s purely subjective. Whatever, loops work well for me.
I was tempted to try 5/8th wave verticals until I read a paper by W4RNL modelling them against quarter waves and vertical dipoles. The improvements in gain and low take-off angle just don’t seem worth it. I’m sure multi-element vertical beams would be better.
One day I’ll have to measure my ground conductivity and dielectric constant: meanwhile I use an estimate based on the ARRL Antenna Book’s values for my type of soil (around 6-9 inches of topsoil on a clay base on a forested hilltop), namely 5 to 6 milli-Siemens per metre conductivity and dielectric constant of 13.
My first antenna experiment in ZL was simply to add additional wires in parallel to the existing 40m quarter wave vertical, using the same coax feed and ground plane. I added 30m and 80m quarter waves - the 80m one makes an inverted-L. They seemed to work, after a fashion, but were noisy on receive. That’s a FAIL.
I’m considering an array of quarter wave LF verticals sharing a common feeder, earth mat and tree top support:
The design is based on a receiving antenna shown in The Radiotron Designers Handbook of 1953. The 160m vertical will be an inverted L as even our tallest trees are not quite 40m - more like 30m at a guess. The earth mat will be a combination of deer fencing and wire radials. The antennas will be separated by a convenient distance along the cord - a few metres each (I’ll lay the lines out on the ground to set it up). I could use two cords from the top, alternating the verticals to spread them laterally as well as along the cord, but the single cord design looks easier. I’m hoping the magic of resonance will effectively feed one vertical per band, although on 40m the topband vertical will accept some RF so the match may need adjustment on 40m and the pattern may be high angle - in which case I’ll just have to try something different (an L-match or low-pass filter feeding the 160m vertical maybe, a high pass filter for the 40m vertical, a remote relay at the base or a completely separate 40m antenna).
Multiband fan vertical design (as yet unproven!)
Yet another possibility is a quarter-wave vertical/L for 160m, end-fed on 80m with a relay-switched matching unit such as those described by AA5TB.
So many antennas in mind, so little time!
< I’ve been planning 4-square antennas for ages. It took me so long to get around to it that I thought about just buying one from the local Four Square supermarket.
The antenna design is easy enough: four identical quarter wave vertical antennas set at the corners of a square with quarter wave sides. Using the simplest feed arrangement, the antenna fires across the diagonals giving one of four directions: it needs a negative phase shift on the forward antenna relative to the sides, while the rear antenna needs a positive phase shift. The pattern is cardioid.
Patrick TK5EP published a simple circuit for a 4-square hybrid coupler using three DPDT relays and a 3-core control line to switch directions. I created an Excel spreadsheet using textbook formulae and the manufacturer’s AL values for various Micrometals powdered-iron toroids to confirm TK5EP’s component values for 40m. By my calculations, T300-2 cores give exactly the right inductance and can handle more power than the T200-2’s favoured by TK5EP ... but for practical reasons to do with the length of the fibreglass poles I had on hand, I started with a 30m version to prove the concept.
The tin roof of my workshop makes an excellent groundplane, roughly 10m square. Originally it was rectangular, so I added a tin roof woodshed to make it squarer ... and coincidentally I now have somewhere to store dry firewood for the winter.
The antenna elements are wires, attached to fibreglass roach poles using rings of heatshrink tubing. The poles are a push-fit into surprisingly strong adjustable angled base fittings made to hold Sky satellite dishes, a very convenient arrangement. The purple wire is the earth connection to the coax outer, relying on metal to metal contact of the fitting to the galvanized steel shed to couple it in to the main roof area.
The calculated inductance values in the hybrid coupler on 30m require 8 turn coils on T300-2 cores, but for some as-yet unknown reason, my shiny new LCR meter from Hong Kong measures them at more than twice the target inductance (the calculations and inductance values are correct, but the meter is wrong, although it measures small potted inductors of a similar value correctly). The coupler needs two 156pF capacitors: I could only find 100pF HV capacitors in my junk box, so added some coax tail capacitors in parallel in the first version.
< Here’s the hybrid coupler phasing/switching box mounted under the shed roof. The toroids are cable-tied to a chunk of PVC pipe to keep them in place. The device on the left is a 50 ohm ceramic power resistor bolted to an over-sized heatsink to dump lost power due to imbalances in the system.
I got about 2 or 3 S-points difference front-to-back and signals are about 1-2 S-points lower off the sides. At last I could tell whether 30m signals from Europe were coming via the long or short path! Direction switching was instantaneous of course.
Unfortunately, erecting a tower next to the workshop messed up the 4-sq beam pattern and matching so eventually I reverted to a single quarter wave vertical ground plane instead, and that does just fine.
In the Antennex article “Adjacent band quad behavior”, LB Cebik W4RNL used antenna modelling to calculate and optimise the characteristics of two-element two-band (hence “2x2”) nested spider quads for various combinations of the upper HF bands. In a follow-up Antennex article “Sneaking Up on 2-Element Common-Feed Quads - Part 3: Dual Band Quad Beams With Common Feedpoints” W4RNL adapted the design for a common feed located at the normal feed point half way along one side of the smaller quad.
This arrangement (below) slightly distorts the driver of the larger quad and affects all the design figures, but modelling shows minimal effects:
The calculated free-space gain (around 7dBi) and front-to-back ratio (20-30dB) are quite respectable for such a simple design. Azimuth plots show reasonably clean patterns predicted on both bands.
Feedpoint impedances are calculated to be around 100 to 125 ohms being mostly resistive with just a little reactance. Although the author suggests using a section of 75 ohm line for matching , a 2:1 toroidal balun at the common feedpoint would - I think - present a reasonable match to 50 ohm coax.
Here are the element dimensions from W4RNL’s follow-up Antennex article, with the metric equivalents:
Using the spider quad design (i.e. spreaders radiating from the centre point of the array), the spreaders would need be about 10 feet (3m) long. I should be able to fabricate a spider centre using a short boom of square steel box section with angle-iron supports welded on at 62 degrees to attach the support arms. To attach the antenna to a round steel mast (a 2” diameter steel scaffold pole in my case), the end of the mast will need to be grooved to fit the corner of the box section steel, and then welded on: in practice, I’ll probably weld on a short stub of smaller diameter steel pipe that will sit snugly inside the main mast, with a locking pin through the main mast and stub to stop the antenna turning relative to the mast.
Big parafoil kites are ideal for lifting wire aerials, given sufficient, steady wind and plenty of space. Parafoils are lightweight, spar-less, nylon kites that fold up into a small rucksack. Their aerofoil section (rather like a skydiver's parachute) gives loads of lift and they are fairly static in the sky (no good for aerobatics or fighting, ideal for hoisting aerials). My 5 ft-wide parafoil kite will lift a top-band quarter-wave wire in a decent steady wind (Beaufort force 3 or above), and I've used it to hoist vertical dipoles, inverted-Vees etc. using slotted plastic twin-feeder rather than coax (it's lighter and lower loss). In fact, it gives so much lift that it's a real handful in a strong breeze (force 5+) - a struggle to pull it down. For lots more ideas on kite and balloon-hoisted LF antennas, visit G4VGO’s site.
There’s a lot of information (and some misinformation!) circulating in amateur circles about radials for verticals. Much of it is based on decades-old research conducted for commercial broadcasters, who have the space and resources to install and maintain over 100 radials per antenna. A fair amount of more recent advice draws on purely theoretical studies using antennal modelling software ... which presumably also draws on the decades-old research just mentioned. Quite a lot of what we read (... including my own musings ...) is essentially anecdotal (“It works really well: I work loads of DX!”). Unfortunately rather few hams have done the legwork to demonstrate, conclusively, what does or doesn’t work in a typical amateur setting, or to answer very common yet basic questions such as:
How many radials should I put down?
How long should they be?
Should I lay them on the surface, bury them or elevate them?
What if I can’t lay them out symmetrically?
So, it’s a refreshing change to read a scientific study of radials for vertical antennas by a dedicated amateur, Rudy Severns, N6LF. It’s obvious from Rudy’s excellent articles in QEX that he knows his stuff. He has carefully researched the professional and amateur literature and then designed and painstakingly conducted the controlled experiments to check out various theories in practice.
If you have the time and interest, I recommend studying all 7 of Rudy's articles in the series. If not, here are the takeaways :
Use between sixteen and thirty-two ¼λ radials on the ground , or at least four elevated ¼λ radials.
If you don’t have the space for ¼λ radials, lay down a larger number of shorter ones.
The shorter your antenna, or the poorer your soil, the more you depend on the ground system.
A surface-radial ground system will affect the resonant frequency so you may have to adjust the vertical height to compensate.
Aside from the earth system, work hard at making the antenna itself more efficient. In other words, use high-Q loading coils, use top loading to minimize the size of loading coils, minimize conductor losses and so on.
Note that sixteen is not a magic number for on-ground radials. The experimental data indicate marginal improvements with more radials but rapidly diminishing returns probably make the effort pointless above about 32 radials and, as the last bullet suggests, we are probably better-off optimising other parts of the system (such as the radiator, the feeder, the rig, the operator and the QTH - plenty of improvement opportunities!) rather than the radials.
Let me say that again: unless you are absolutely desperate to squeeze the last tenth of a dB out of your earth mat, there is no practical value in going beyond 32 radials. Those guys who diligently lay out 100+ radials per radiator will do their utmost to convince you that it was well worth the effort, and in psychological terms they may be right but, scientifically-speaking, they are somewhat deluded. Just because 120 radials happens to be the numeric standard in broadcasting doesn’t make it appropriate, necessary or worthwhile for amateur stations.
If you use too few on-earth radials (e.g. just 4), their lengths become critical - in other words they are resonating, which leads to the counterintuitive finding that reducing their lengths to hit resonance may actually improve their efficiency!
Experiments simulating installations where there is no room for ¼λ radials right around the base of a vertical indicate that symmetry is fairly important. Efficiency is slightly reduced if one quarter of the circle is empty, and losses mount to as much as 3 dB (half your power!) if you can only lay radials in a semicircle. However, substituting the missing radials with more, shorter ones in the directions that you can lay radials offsets the effect a bit.
Another fascinating insight from Rudy’s experiments is that numerous factors affect the effectiveness of the radials, including for example the soil conductivity which varies with geology, moisture levels and band. Unless you can measure and control these factors, theoretical calculations from antenna modelling may not hold true in real installations, hence the value of careful experimental studies like Rudy’s.