For a general introduction to Small Transmitting Loop antennas (STL, a.k.a. "Magnetic Loops"), incl. coupling methods, please see my 80-20 STL page.

Latest page update: September 2022 (replaced motor to reduce the capacitor shaft rpm)

Previous page updates: 1 May 2022 (added results from preliminary 2-turn vs 1-turn STL tests)

©2021-2022 F. Dörenberg N4SPP/F4WCN, unless stated otherwise. All rights reserved worldwide. No part of this publication may be used without permission from the author.


My motivation for adding this page. My 1-turn loop antenna (ca. 2 m diameter ) actually works quite well. Though electrically small, it is physically large (compared to my own size). It is also quite heavy, and therefore awkward to handle. To maximize performance in the direction that I am interested in, I have to lift the antenna above the roof line with the telescopic mast on my terrace. I cannot leave this antenna permanently installed on the mast. Installing the antenna requires me to get up on a step ladder and maneuver the antenna. On several occasions, I have almost fallen of the ladder, or of my pergola, with the antenna! This antenna also has a significant wind load.

A 2-turn antenna with the same total conductor length, would be significantly smaller, and easier to handle. However... conventional antenna theory implies that a loop's radiation resistance (simply put: the part of the loop impedance that radiates rather than dissipates) is proportional to the square of the surface area that is enclosed by the loop - independent of the actual shape. Going from a 1-turn to a 2-turn loop with the same "copper length" would reduce the radiation resistance by a factor of four. So, the already very small radiation resistance (several dozen milliohms) would become even smaller. At the same time, the loss resistance would actually increase due to coupling between the two turns and "more copper near ground". Combined, this would significantly reduce the loop's efficiency, and therefore the performance.

The conventional formula for "radiation resistance" (Rrad) includes a factor N2, where N is the loop turns number. This suggests a 4x increase of Rrad for N = 2. However, two turns with same total radiator length --> diameter D is halved, which - via the term D4 - implies a reduction of Rrad by a factor of 16, or an overal reduction of Rrad by a factor of 16 / 4 = 4.

Vs. increased losses, e.g., due to proximity of the loop turns?

How / to what extent is main loops self-inductance affected by N (conventional N2 formula does not take into account all sorts of effects such as proximity between adjacent turns and RF frequency - use the "RF Inductance Calculator" by ON4AA for my N=1 and N=2 loops at 80-40-30). Implication for capacitor size? Confirmed by measurement? Can the current around the two loop turns still be considered constant, as in same-inductor-length STL? Q and voltage across the capacitor? For lossless loop, Q = SQRT(L/C) / Rrad --> if L 4x larger (not realistic per ON4AA calculator), hence --> the C required for a particular fres is 4x smaller (TBC),  and Rrad 4x smaller, then Q increases 32x --> BW 32x smaller????

This is quite discouraging for conventionally minded people. It is also consistent with one of the most important fundamental laws of nature: Conservation of Misery!

Nonetheless, I would like to be able to weigh the actual reduction in performance against the improvement in compactness, weight, wind load! I am primarily interested in "DX" performance, not NVIS and local ragchew. An extensive web etc. search on this topic basically came up with not much practical evidence, in particular no side-by-side comparisons of actual antennas. Also, a 2-turn loop should be less expensive: it has a higher self-inductance, which should require a smaller (in terms of pF, size, weight, cost) vacuum capacitor for tuning down to 80m.

This is why I am going through the trouble of building and testing a 2-turn loop - without cannibalizing my 1-turn loop. So I can make comparative performance measurements. Construction and test results are documented towards the end of this page.

Mag Loop

Fig. 1: This is what it is about: my 1-turn and 2-turn loop antennas side by side - with myself as size reference

(I am about 1.8m = 5 ft 9 inch tall)

The bottom line conclusion of my build-and-compare efforts is quite positive. It reminds me of the more than 100 years old encouraging saying: "That may work in practice, but not in theory!". But getting to that point has not been a smooth path...


Let's jump straight into te construction. A couple of years ago, I bought a standard 20 feet "copper coil" at a large Do-It-Yourself store - for a future project. Total length 20 ft = 6.1 m. I used another such coil for my 1-turn loop. The tubing has an inner diameter (ID) of 1/2 inch (12.5 mm) and an OD of 5/8 inch (16 mm). It weighs 5.75 lbs (2.6 kg). It is made of soft copper. This is also called "annealed" tubing, as it is heat-treated after the tubing is drawn in the factory. This relaxes the stress that is caused by the tube-drawing process. This is very important. You can almost bend soft copper tubing by hand, if it has a reasonably small OD. For hard-drawn copper, you need a heavy manual pipe bender, or - for a clean job - a professional hydraulic bender.

To make a nice, round loop without professional bending tools, you need a bending jig. It has to be somewhat smaller than the specific loop diameter that you want. I reserved 6 inch (15 cm) at each end of the 20 ft tubing, for a bent 90° connection to my tuning capacitor. This leaves 19 ft (5.8 m) for the actual loop, or 9½ ft (2.9 m) per loop turn. I.e., a loop with an inner diameter of about 3 ft (92 cm). Upon bending, tubing tends to spring back a little, so I designed my jig for an inner diameter that is about 2 inches (5 cm) smaller than that.

Note: if your copper tubing is new and nice & shiny, and you want to keep it that way (at least for a while): don't touch it with your bare hands (I use very thin touchscreen / smartphone gloves)! Otherwise the copper will get tarnished very quickly. Contrary to popular belief in some circles, this does not affect performance of a loop below VHF frequencies, as long as the contact surfaces between the loop and the tuning capacitor are corrosion-free. See here.

The photo below shows the tools that I used to make my wooden jig. At the far right in the photo is a standard "manual rotary draw bender" (F: "cintreuse de tuyau", "pince à cintrer", D: "Rohrbieger"). It has a so-called "die" that matches the outside diameter of the tubing or pipe - 16 mm in my case. As stated above, I will bend the ends of the tubing 90°. I want nice bends with a relatively small radius. This can only be done cleanly with a pipe bender. It clamps the straight tubing against a concave bender-die, and pulls the tubing around the die - while maintaining a constant tube diameter. I.e., without collapsing or wrinkling the tube. You cannot do this by simply pulling the tube around a small round shape small by hand!

Mag Loop

Fig. 2: The basic tools I used to make my jig (variable speed power drill, jigsaw, vise-grip clamps) and a "household" pipe bender

I made the loop bending jig with pieces of scrap wood that was left over from a project around the house. The jig must have a "channel" that holds the tubing. My tubing has an OD of 16 mm, so I used 18 mm thick particle board. The pieces are fixed together with about two dozen 5x35 mm self-tapping drywall screws ( = self-drilling plasterboard screws). Note that the screw length is just less than twice the board thickness, so the screws will not poke out the bottom of the jig base plate, and damage whatever is underneath (such as the table).

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Fig. 3: Pieces of the wooden bending jig (left) and the assembled jig (right)

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Fig. 4: The jig is clamped onto a heavy table

Jigs and benders are normally used with straight tubing or pipe. My copper tubing was rolled up into a small tight coil - yes, much easier to transport than 20 ft / 6m straight tubing! The ends of such coils are normally straight - which is good - because the coil was made of straight tubing. I first carefully uncoiled about 1½-2 ft (≈50 cm) of the coil. It doesn't have to be straight - just straighter than the curvature of the jig!

Mag Loop

Fig. 5: The 16 mm wide starting end of the jig (left) and the "groove" (channel) that holds down the tubing while pulling it around

The straight(ened) end of the tubing is inserted into the starting end of the wooden jig (from the top-left in the left-hand photo in Fig. 5 above), until about 6 inch (15 cm) sticks out. This piece will later be bent 90° to attach the capacitor. The uncoiled part of the tubing is then pulled completely into the channel of the jig, all the way around the entire jig. Then, the now curved part of the tubing is loosened a bit from the jig channel, and pulled through the feed-end of the jig. Then, the next section of tubing is carefully straightened a bit, and pulled all the way into the entire curved jig channel. This is repeated until the entire coil has been reshaped. The resulting loop looks quite nice, see Fig. 5 below. It would have been entirely impossible to make it this round without a jig (or paying a professional machine shop too much money to do the work for me). Bending the 90° turns at the ends of the loop did require some fiddling, and learning how to set up the pipe bender for making the bend at the right spot.

Mag Loop

Fig. 6: The soft copper coil - reshaped into a 2-turn loop with bent ends


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Fig. 7: My 2-turn loop without the tuning capacitor, suspended for measurements

Before making the attachment brackets for the vacuum capacitor, I was anxious to take some simple measurements with my miniVNA antenna analyzer. In particular the self-resonance frequency. Without the tuning capacitor, this is inherently the highest possible fundamental (i.e., non-harmonic) resonance frequency that can be obtained with this loop - at the specific installation location and height. Adding a tuning capacitor will always result in a lower resonance frequency: the capacitor has a non-zero minimum capacitance - at least several pF - and mounting it onto the loop-ends probably also adds some stray/parasitic capacitance.

I did not change the pitch of the loop turns from when it came out of the jig: about 3-4 inch (8-10 cm). Note: coil "pitch" is normally defined as the on-center distance between two adjacent conductor turns. However, sometimes the separation distance between two adjacent conductor turns is meant. This is not always explicitly stated in coil inductance calculators and in antenna simulation tools that support definition of a helix.

Mag Loop

Fig. 8: Coil dimension parameters, including "pitch"

I used simple unshielded coupling loops, like the one I use with my 1-turn loop antenna - which has with the same overall circumference as this 2-turn loop. Coupling loop #1 had a circumference of 123 cm (4.4 ft), i.e., a diameter of 39 cm (1.28 ft). Coupling loop #2 was slightly smaller: circumference of 100 cm (3.4 ft), i.e., a diameter of 32 cm (1.04 ft). These experimental coupling loops were made of stiff solid household installation wire, mounted directly onto the BNC connector of the antenna analyzer - no coax. In both cases, the self-resonance frequency was around 17950 kHz. The coupling loops were suspended between the two turns of the main loop, see Fig. 6 above. Their position could easily be adjusted for a minimum SWR of 1.14, which is excellent. With the smaller coupling loop, this best SWR was obtained with the coupling loop coplanar with the main loop. The larger loop had to be rotated about 45° out of the plane of the main loop. This means that it is a bit too large.

My 1-turn loop also has a circumference of 20 ft (6.1 m), i.e., a diameter of 6.37 ft (194 cm). A standard 1/5 size coupling loop would have a diameter of 1.2 ft (37 cm). My simple measurement shows that the coupling loop of a 2-turn loop should basically have the same size as a standard size coupling loop of a 1-turn loop with the same overall circumference.

What is the optimal pitch of a 2-turn loop, or a multi-turn loop in general? I have not been able to find any theoretical basis in available literature. In the few documented implementations that I have come across, the pitch is based on "size of standard tube-clamping spacers", "visually pleasing proportions of the pitch vs. the loop diameter", "at least 5x conductor diameter" (which would be 5x16 mm = 8 cm in my case), and 7.5x conductor diameter (ref. 1A). Of course, a multi-turn loop is just a single-layer cylindrical solenoid air-core inductor. And "optimal" has to be defined first. Factors: stray capacitance (primarily between adjacent turns), proximity effects, loss...


Expecting loop inductance to be at least 2x that of my "same circumference" 1-turn loop --> need only half the tuning capa range of  --> 5-250 pF. So, I acquired one. It is about half the size of the big "bottle" of my 1-turn loop, and 1/3 the weight of the latter:

Mag Loop

Fig. 9: My vacuum capacitors: (top) 10-500 pF, 10 kV, 36 revs, 2.2 kg; (bottom) 5-250 pF, 5 kV, 24 revs, 0.73 kg

(The two photos are to the same scale)

Mag Loop

Fig. 10: Capacitance vs. shaft revs of my 10-500 pf / 10 kV and 5-250 pF / 5 kV vacuum capacitor

Curve is perfectly linear between min & max capacitance; remember that resonance frequency of an LC-circuit (such as loop + tuning capacitor) is proportional to the reciprocal of the square root of the capacitance. So, the resonance freq does not vary linearly with the capa revs! The capacitor shaft can make 24 revs, but the capacitance effectively only changes over 15 revs. So, the motor drive for this capacitor should also be able to make at least 15 revs.

Copper tape mounting brackets. For connecting the cylindrical ends/electrodes of the vacuum capa to the ends of the copper tube loop - same approach that I used for my 1-turn 80-20 STL (link; Fig. 75, 76.).

Diameter of vacuum cap ends/electrodes: 52 mm -- > circumf 163 mm, add ca. 2 cm at each end for taps --> need 20 cm (8 inch) strips. Soft Cu strips: 200x15x0.8 mm. They are a tad thin, would have preferred 1.0 mm, as for my large vacuum cap. 2x2 rectangular steel washers ["stretchers"], customized (18x15x2, offset hole --> 2 hole-to-edge choices, cut out of a 2 mm thick flat bracket from the junkbox ). 2x stainless steel bolt 6x20 mm, with hexhead for adjustable or socket wrench, + 2x stainless lock nut

Mag Loop

Fig. 11: Capacitor mounting brackets - drilled & preshaped strips + rectangular washers, M6 bolts, M6 lock nuts

For pinching the ends of the loop, I use locking pliers (trade names include Vise-Grip™ and Mole-Grip™) because you can exert very large force with them. Drilling 6 mm holes, deburr, ensure completely flat (smoothing/filing if necessary).

The inside of the copper brackets and the pinched ends of the copper loop must be cleaned until they are shiny. I either use standard household copper/brass cleaning cream and a cloth, or - what I actually prefer - a small piece of kitchen scrub sponge and some.... toothpaste! Then rinse thoroughly. Sometimes I also boil them in water for a couple of minutes. Once the surfaces are clean: no more touching the inside surface of the brackets! I clean the silver-plated electrodes of the vacuum capacitor with standard household silver polish (you may have to repeat this several times to get all the oxide off), then thoroughly clean with a sponge and water. Again, do not touch the cleaned electrode surfaces anymore!


Made 4 spacers. Copper diameter 16 mm, used some 20 mm diam OD PVC conduit, left over from another project. Number of spacers is to be minimized, to minimize inter-turn effects / Q during high humidity, rain, etc.; already have 2 spacers: the vacuum cap and the attachment to the PVC mast. Used standard tie-wraps - black ones, because white ones do not last very long in sunlight.

Spacers are dimensioned for 8 cm = 5x diameter of the Cu tubing. Why?

Components / material for the mast & loop support:

  • Mast (that slides onto my heavy umbrella stand and onto the mast insert of my telescopic mast): standard PVC tubing, 63 mm OD, length 125 cm (loop diameter + 30 cm)
  • Loop support "gallows": thick-wall PVC tubing, USA type "Schedule 40 - above ground / underground non-metallic conduit" (0.84 inch OD (21.5 mm) and 0.622 inch ID (5.8 mm), length 1 ft (30 cm).
  • Due to its 3 mm wall thickness, this tubing is very stiff - which is exactly what I want for suspending the loop on the side of the mast.
  • With the capacitor at the bottom, the copper tubing at the top of the loop is at 1/2 and 1-1/2 x inter-turn spacing + 1 tube diameter from the mast. Add mast diameter + a couple of cm --> support tube length has to be > mast OD + 2x Cu tubing OD + 1-1/2 inter-tube spacing = 63 + 2x16 + (3/2)x80 = 215 mm --> 25 cm incl. some margin.
  • PVC tube clamps, 3 for clamping the loop to the "gallows" and to the mast.
  • I use standard clamps intended for 14/15 mm OD tubing. They fit very snugly onto the 16 mm OD copper tubing of my loop.
  • The clamps have an integrated M6 nut, so I need two M6x30 bolts + 6 mm lock washers for attaching two clamps to the "gallows", and one M6x80 bolts + lock washer for the attaching the bottom of the loop to the mast.
  • Inter-turn spacers (at least 2, distributed around the loop)
  • Thin wall PVC tubing, 20 mm OD, length: 4 inch (10 cm) each
  • Black tie-wraps (white ones are not UV-resistant and become brittle very quickly outdoors), 2 per spacer

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Fig. 12A: Top end of the PVC mast with PVC support "gallows" for the loop

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Fig. 12B: Attachment of the top & bottom of the loop turns with tube clamps

Choice: clamps upward on top/upward or below/downward the PVC "gallows" ???

Mast: my standard (fits snugly on my umbrella stand and the custom insert of my telescopic mast.

The on-center spacing of the capacitor electrodes is 10 cm (2 inch). So, I decided to go with a 5 cm (2 inch) pitch. Two clamps at the top, capacitor across the tube ends --> decided to add two spacers


A standard coupling loop has approximately 1/5 the diameter of the main loop.  Some use 1/6. But what is the standard for a 2-turn loop? With a 1-turn STL, the coupling loop is typically installed in the plane of the loop, and the distance between the main loop and the coupling loop is adjusted as needed.  With a multi-turn STL, the main loop is not aplane but has a cylindrical volume. So the position of the coupling loop is 3D instead of 2D: one more parameter to adjust!

To be able to quickly explore various coupling loop diameters, I got several 1 m sections of thin straight brass tubing at the local do-it-yourself store. It has an outer diameter (OD) of 4 mm, and an inner diameter (ID) of 3 mm ID. I mounted a "female-BNC to banana plug" adapter to the tip of a 10 cm (4 inch) piece of a wooden broomstick (diameter 23 mm, about 1 inch). That places the coupling loop within the volume of the 2 turns of the main loop. The wooden rod is attached to a PVC clamp for the standard 63 mm OD PVC tube that I use as mast for the anenna:

Mag Loop

Fig. 13: Experimental coupling loops

Mag Loop

Fig. 14: Mast attachment for the experimental coupling loops


  • The brass tube ID is 3.0 mm, but the tip of the banana jacks has an OD of 3.1 mm. I increased the ID of the tubing ID to 3.1 mm by careful drilling with a 3.1 mm drill bit. The jack tips can then be inserted several mm into the tubing and be soldered. This is rigid enough for experimentation purposes. I made 4 exchangable brass loops with 16, 19, 24, and 31 cm diameter. This compares to the 95 cm diameter of the 2-turn loop and ca. 195 cm diam of my 1-turn loop.
  • The BNC adapter is rigidly fixed to the broomstick stub with two cable ties.
  • for the coupling loop, contact/loss resistance (e.g., between the between the banana plugs of the BNC adapter and the banana jacks soldered to the brass tubing) is not critical (unlike losses in the main loop).

Which coupling loop did I select? I eventually settled for a coupling loop with a diameter of 16 cm (6.3 inch),: close to 1/6 of the main loop diameter.

I used the banana plug and BNC-adapter approach for the final version of an easily-removable coupling loop. A "bird house" made of pieces of PVC L-profile provides weather protection. A small insert made of three sandwiched-and-glued pieces of PVC closes the slit on the mast side of the birdhouse.

Mag Loop

Fig. 15: "Bird house" for weather protection of the BNC adapter of the coupling loop

The optimum position of the coupling loop is sensitive to installation height of the antenna and the operating frequency. I need the flexibility of using the antenna at different positions on my terrace and above my telescopic mast. So, I absolutely need motorization of the coupling loop. See this section.

I also tried a ferrite ring transformer coupling, instead of a coupling loop. Ferrite ring: FT-240-31, i.e., OD = 2.4 inch (6.1 cm), made of "31" material. With the loop in my umbrella stand on the terrace, the loop bottom about 1 m above the terrace floor, the ferrite ring installed half way around the loop, i.e., between the loop ends, exactly between the capcitor connections ( = equivalent to the neutral point, opposite the tuning capacitor of the 1-turn loop), standard 1.5 mm2 solid copper household installation wire with PVC insulation (European type H07V-U). With 17 wire turns, evenly spread around the ring, I got SWR = 1.53 around 3590 kHz and SWR = 1.03 around 7080 kHz. With 19 turns, I got and SWR = 1.53 and 1.23, respectively. With 21 turns, I got SWR = 1.1 and 1.47, respectively. So: no single number of turns to cover both bands! The required number of turns is quite sensitive to loop installation hight / position. Note that this is very similar to the results obtained for my large 1-turn loop with ferrite ring transformers: only useable over a frequency range of about 750 kHz, i.e., for single band operation. See here. To cover the 80 & 40 m bands for experimental purposes (at least the portions of those bands that I am interested in), I put 17 + 4 wire turns on the ferrite ring, and used a simple household terminal block to select the 17 vs. 21 turns:

Mag Loop

Fig. 16: Selecting 17 vs. 21 wire turns with a terminal block and a BNC adapter

(shown with 17 + 4 = 21 turns connected to the BNC adapter)


Drive folded back, parallel to longitudinal axis of varicap; more compact than fully in-line, as I built for my 1-turn 80-20 loop.

Diagram. Design / parts list. Slide(r) potentiometer with linear taper instead of 10-turn potentiometer - no need for motor gearbox with 2 output shafts. Retain POM isolation shaft. End-stop protection (though the capa may be able to handle the motor torque at the ends of its travel).


  • Motor: 12 volt DC, with integrated down-gearing to 20 rpm, Ø 6 mm output shaft, torque rating not specified.
  • The 20 rpm speed is the unloaded speed for a 12 VDC supply. I use a standard "amateur radio" commercial power supply, so it outputs 13.8 VDC. This increases the unloaded motor speed to 24 rpm.
  • My varicap has a 24 revs range, of which 15 revs actually change the capacitance, see Fig. 9 above. I would like traversing the 15 rev effective range to take about 45-60 sec. Based on this, I decided to go with a 15:20 down-gearing ratio between motor and capacitor.
  • Choice of drive speed (motor + down gearing): effective capa rev range (see Fig) + cover that range in about 1 min.
  • Note: the output shaft of this motor is not centered on the round surface of the gearing (see Fig. XX). This makes it a bit awkward to install the motor on an L-bracket such that the shaft is aligned with lead-screw. To adjust the height of the shaft, either the height of the bracket has to be changed, or the motor housing has to be rotated. This is a bit of a hassle. With a centered shaft, only the height of the mounting holes has to be adjusted straight up or down.
  • Backlash is "play" when changing direction. This undesirable in high-precision positioning systems. I have measured a backlash of 4° shaft rotation at the output shaft of the gear box. The gear box has a very large gearing ratio, to get down from several 1000 rpm to 20 rpm. This requires a multi-stage gear box, and each gear stage adds backlash. Only very expensive gear boxes have anti-backlash (ABL) gearing, which is beyond the typical amateur radio budget.
  • Isolation shaft between motor and capacitor not needed if using a timing belt between the two gear pulleys that does not have embedded steel reinforcement cords (Kevlar is OK; polyurethane belts usually have steel, which will lead to arcing with high voltage across the tuning capacitor, see Fig. 100 on the 80-20 page).
  • Flexible shaft coupler, 6 mm / 8 mm bores, 19x25 mm LxD; connects motor shaft to isolation shaft. Of course, a ceramic shaft works fine too.
  • Isolation shaft, Ø 8 mm POM (acetal, polyoxymethylene; this is very strong polymeric resin with trade names such as Delrin, Celcon, Duracon), xxx cm long. has a high dielectric strength. A 20 mm long piece of clean, smooth, dry POM should easily provide well over 10 kV isolation.
  • Flexible shaft coupler, 8 mm / 8 mm bores, 19x25 mm LxD; connects isolation shaft to lead screw
  • Lead screw assembly:
  • Lead screw: stainless steel, Ø 8 mm, 2 mm pitch, length: standard 200 mm (8 inch), reduced to 115 mm (≈ 4.5 inch); eBay "linear lead rod shaft".
  • Brass lead-screw nut (typ. comes packaged with the lead-screw)
  • The flange of the nut has four non-threaded holes. I threaded the holes with an M4 tap
  • M4 screws, for fixing flange of leads-screw nut to the slider block.
  • Two pillow-block ball bearings with Ø 8 mm bore, to support the lead screw.
  • Spacers (for raising pillow blocks, if necessary) - TBC
  • Slider block (PPE, 45x30 mm WxH; width the same as the length of the OD of the lead screw bushing), to be mounted onto the lead screw bushing.
  • Hole for bushing not drilled until after confirming final height of the pillow-blocks and, hence, of the lead screw
  • ACTUALLY:  Some (1-2 mm max) extra height below the holes, bottom of the block to be adjusted with rasp & file for low-friction slide without creating a gap that adds any significant rotational backlash/play of the lead screw.
  • Two micro-switches, to detect reaching the end of the travel of the slider block. The micro-switches must be "single pole, double throw" (SPDT) types. I.e., with three contacts: common, "normally open" (NO), and "normally closed" (NC). The switches are not only used to interrupt power to the motor, but also to enable changing the motor direction away from the end-stop (which is rather practical).
  • Two general-purpose diodes, used in combination with the micro-switches, to enable changing motor direction after reaching an end-stop. They should have sufficient forward-current capability to handle the max motor current (1 Amp in this case). I use 1N4007 diodes, as I have plenty of those in my junk box.
  • Additional 15:20 down-gearing of the 20 rpm nominal motor speed to 15 rpm at the capacitor shaft (yes, I could have used a 15 or 10 rpm motor and 1:1 gearing).
  • Gear (pulley), aluminium, 8 mm Ø bore, 24 mm OD, 15 teeth, 0.2 inch pitch (5.08 mm), 11 mm between the flanges. To be mounted on the 8 mm Ø lead screw.
  • Gear (pulley), aluminium, 10 mm Ø bore, 20 teeth, 0.2 inch pitch (5.08 mm), 11 mm between the flanges; 45 gram (1.6 oz). To be mounted on the 10 mm Ø shaft of the capacitor.
  • After arc damage & large freq shift & Q reduction: got polycarbonate timing pulleys (15T, 30T) with aluminum insert. Solved the problem???
  • Timing belt (a.k.a. toothed belt, synchronous belt),10 mm width, 0.2 inch pitch (5.08 mm), 41 teeth, i.e., "82 XL".
  • My measurements suggested I needed either a 40 of a 41 teeth belt. A slightly long belt could be accommodated by the height of the varicap support cradles (see next item). A slightly short belt would not work. The 41 teeth belt turned out to be perfect.
  • Use a belt that does not have embedded steel reinforcement cords - Kevlar and fiberglass! Many polyurethane belts have steel cords, which will lead to arcing when high voltage across the tuning capacitor occurs (i.e., at the antenna's resonance frequency), see Fig. 100 on the 80-20 page.
  • change 15:20 --> 15:30 gear ratio = factor 1.5 change --> capa drive speed & range reduced by factor 1.5 (easier precis tuning) but freq range by factor SQRT(1.5) = 1.22 from 3.5-11 MHz --> 3.5-9 MHz --> antenna from “ 80-30” to “80-40”.
  • Two support cradles for the capacitor. I made them out of a piece of PPE. See Fig. ??? below.
  • I used a Ø 55 mm hole saw - slightly smaller than the 58 mm diameter of the capacitor's black end-cups of my capacitor's glass cylinder. Next, I used a large so-called "half-round" rasp, to increase the hole diameter to a tight fit on the end-cups. Then I cut the PPE piece in half, to get two cradles. Final adjustment of the cradle height was made after selecting the length of the timing belt.
  • Note: do not use a hole saw at high rpm with PPE - it melts the PPE, which fills the cut back in, and makes the saw appear "dull".
  • Mounting plate: 250x100x11 mm PPE material (polyphenylene ether, a stiff polymer "plastic"), cut out of an inexpensive PPE kitchen cutting board.
  • Miscellaneous:
  • Two tie-wraps, black (white ones are not UV resistant!), width x length ????. For fixing capacitor to the support cradles.
  • Ethernet chassis connector, for the ethernet cable to the remote control box.
  • Slide(r) potentiometer (for position feedback to the remote-control box), must have a linear taper - i.e., absolutely not a logarithmic "audio" taper !!!)
  • The lever must have a sliding range/travel of at least that of the lead screw nut for the effective rev range of the capacitor. In my case:  2 mm pitch x 16 revs x 15:20 down-gearing + width of the sliding block (??? + width of nut flange?) + margin = 43 mm + ???? = 1.7 ??? inch, plus margin. I used a mono ALPS brand model with 60 mm travel.
  • Resistance: at least 10 kΩ. The one that I use is 20 kΩ.
  • I soldered small copper L-brackets to the ends of the potmeter housing, to be able to mount the potmeter onto the base plate with countersunk M3 screws.
  • Note: the potmeter that I got, has a small bump on one of the long sides, to mark the center-detent position of the lever. This side of the potmeter has to be "up", otherwise the potmeter cannot lie flat on the base plate. Of course, the small copper brackets have to be oriented accordingly.
  • In the 36 revs motor drive of my 1-turn 80-20 STL, I used a 10-turn rotary potentiometer. This required a motor with 2 output shafts and additional gearing. Here, I used the alternative: attaching the lever of a slide potentiometer directly to the lead-screw nut slider block.

Mag Loop

Fig. 17: Mechanical components of the motor drive

(the actual belt used has more teeth; slider block not shown; micro-switches & diodes not shown, aluminum L-bracket to be adapted to motor)

I do not have a workshop with bench tools. OK, I have a bench vise, but no drill press, bench saw or table saw, ... - only hand tools: electric hand drill, a thin-blade Japanese-style "pull" hand saw (which makes much more accurate & straight cuts than any EU/US "push" saw), a rasp and a file, a thread tapping set, an L-shaped straightedge, and a sliding vernier caliper. Be careful when countersinking a hole in a PPE plate with an electric hand drill instead of a drill press: the drill will tend to suddenly "grab" (especially if the drill bit is still new & sharp) and drill completely through the PPE before you know what is happening!

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Fig. 18: The pre-drilled PPE sliding block, brass lead-screw nut, and M4 screws

(note: the narrow side in the far right image has a hole for the lever of the slide potentiometer)

PPE, 10 mm hole for the bushing part of the brass lead-screw nut; countersunk holes for two M4 screws, and a hole in one side - for the lever of the slide potentiometer.

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Fig. 19: Both sides of the base plate - before installing the parts

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Fig. 20: The cradles for the vacuum capacitor - made of PPE

(the hole is cut with a hole saw and electric drill, height of the cradle is adjusted for belt length, mounting holes are threaded with an M5 tap)

PIX: top & bottom view of populated base plate + 1 image with detail views vs. two full angle views. HOOKUP CONTROL ETHERNET CABLE

The complete drive unit - without the weather protection hood - weighs 1.5 kg (≈ 3.3 lbs).  About half of this is the capacitor. After final adjustments, the drive has a range of 24 lead-screw revs between the end-stop switches. I.e., 24 x (15 / 20) = 18 capacitor shaft revs. This is 20% more than the minimum required 15 revs (which is the effective shaft rev range of my capacitor, see Fig. 9).

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Fig. 21: Top view of the assembled capacitor motor drive

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Fig. 22: Bottom view of the assembled capacitor motor drive

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Fig. 23: Angled views of the assembled capacitor motor drive

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Fig. 24: View of both ends of the drive unit

I re-use the control box of my 1-turn 80-20 loop and the 15 m long "twisted shield pair" ethernet cable to the motor drive. TBC if current limiting resistor (in the motor-stall LED circuit) is correct for this motor's stall current.

Video clip: end-stop to end-stop motion of my capacitor motor drive

©2021 Frank Dörenberg (N4SPP)

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Fig. 25: Capacitor and drive installed on the ends of the loop

As visibile in the right-hand photo above ( = left-hand below), the initial copper strip bracket was not mounted tightly enough around the front electrode of the capacitor. The one in the rear was OK. This did not appear to affect the contact resistance and, hence, the Q and bandwidth of the loop. At least not yet! Better to fix this right away! So, I made two new rectangular washers. This time I made them longer then necessary. As we all know: "It is easier to cut/file/saw something off, then to cut/file/saw something on". I reduced the length to the final size in two fit-and-file steps. Nice and tight, as shown in the right-hand photo below:

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Fig. 26: The initial and final rectangular washers

You may ask: "Why mount the capacitor inside the 2-turn loop instead of on the outside?" Well: 1) overall, it is more compact, 2) to protect the capacitor, 3) ease of adding weatherization (e.g., no need for slits in the sides of the removable hood for the copper tubing). Note that the field strength near the loop conductor is basically the same inside and outside the loop, so that makes no difference. Yes, the motor control cable now has to go inside the loop, but that is just like the coax of the coupling loop - the control cable will be guided upward, mid between two adjacent loop turns.

I thought that the neoprene belt that I used, did not have steel cords, but alas... Effect: at 80 W "key-down", the SWR increased rapidly and then the transmit power was automatically reduced by the transmitter's protection circuit. This suggested heating due to eddy currents somewhere, but due to the quick power reduction, no parts got hot or even warm to the touch. Then I systematically disassembled the capacitor+motor drive (first the cable ties - that were actually very close to the end electrodes of the varicap = high voltage). This slowed down the SWR increase significantly. Now the power stayed high enough long enough to feel and smell heating: the gear belt:

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Fig. 27 The original neoprene timing belt - discoloration and other clear signs of arcing and heating ( = dissipation)

(neoprene belt with steel cords)

I had already encountered such a problem  once before, with the first capacitor drive (with a stepper motor) of my first large 1-turn loop. I removed the belt and the problem was gone - but of course: no motor drive capability. I thought that a rubber belt with fiberglass, polyester, or polyurethane cords would do the job. So, I bought a replacement belt: rubber/neoprene, now with fiberglass cords insated of steel. The impact on SWR and Q was worse than with the original belt:

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Fig. 28: Effect of timing belt material on resonance frequency, SWR, and "Q"

(no re-adjustment of the coupling loop)

I did not even bother to run tests under power. "Loading" the pulley on the capacitor shaft with a rubber/neoprene belt kills the "Q". Note that the DC-motor drive of my 1-turn loop does not have a belt (other than for connecting a position-feedback rotary potentiometer). Instead, is has a short section of POM-material isolation shaft.

The problem was solved with a polyurethane belt and/or at least one non-metal pulley. I also bought fiberglass reinforced polycarbonate pulleys with aluminum insert, to replace the aluminum pulleys.

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Fig. 29: A polyurethane belt with fiberglass cords and neoprene/rubber belts with steel cords and with fiberglass cords

Q of my 1-turn STL is ≈845. As expected (explain!!!!!), the Q of my 2-turn STL is higher: ≈1350. Both are based on the measured 1/2 power bandwidth ( = -3 dB = SWR 2.618 bandwdith). This means that the tuning speed, in terms of kHz per sec, should be correspondingly lower for my 2-turn STL. The initial speed, with max capacitor shaft speed speed = 20 rpm x 15:20 gearing = 15 rpm.

To be measured: achievable shaft speed (with PWM speed controller) for the position-dependent torque/resistance of the shaft ?

With  high: difficult (esp. in 80 m band) to stop the tuning exactly at the best SWR point., undershoots & overshoots. Decided to increase the gearing ratio to 15:30 = speed reduced by 50% by using a larger pulley on the capacitor shaft. This, in combination with the PWM controller, works fine. TBC. Should have used a 10 rpm or even 5 rpm  motor. Of course, compromise between ease of fine-tuning the resonance frequency (not easy, given the very narrow bandwidth thatresults from the high-Q), and time required to tune to a different frequency band.

The motor has a nominal speed of 20 rpm. With the original 15:20 additional down gearing, the nominal speed of the capacitor shaft was 20 x 15 / 20 = 15 rpm. With the PWM motor speed control, this can be further reduced by a lot. However, the lowest achievable speed was still too for comfortably tuning the antenna's resonance frequency exactly to the transmitting frequency. Even short motor activations with minimum PWM setting caused overshoots, due to narrow bandwidth of the antenna. I decided to improve this by increasing the down gearing to 15:30, by using a 30 teeth pulley on the capacitor shaft. Obviously, this larger pulley required a longer belt. I had to increase it from an 82XL037belt to a 92XL037 belt. I.e., 5 more teeth = 5 x 0.2 inch belt pitch = 1 inch longer.

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Fig. 30: Various aluminum and polycarbonate gears wheels that I tried

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Fig. 31: Front view of the motor drive: initial (left; 3:4 down-gearing) and final (right; 1:2 down-gearing)

Increasing the down-gearing ratio decreases the number of capacitor shaft revolutions that the motor drive can make: the number of revolutions that the lead screw shaft can make is fixed: it is limited by the mechanical travel of the linear potentiometer. After installing the large gear wheel on the capacitor shaft, I re-adjusted the drive. WIthout the belt installed, I drove the motor all the way to the end-stop for the lowest frequency. I then adjusted the capacitor to a resonance frequency of 3.52 MHz (i.e., increased from the lowest achievable resonance frequency of 3.44 MHz with this vacuum capacitor), and installed the belt. With this adjustment, the highest frequency was 10.7 MHz (down from 12.7 MHz with the original gear ratio). So, the antenna still covers the 80-60-40-30 m bands.

Update of September 2022: even with the larger gear wheel on the capacitor shaft and the PWM speed regulator at minimum speed, the shaft speed is still high for comfortable tuning: it is not easy to tune without under- or overshooting the SWR dip. At this point, the only remaining simple option is using a motor with with a lower rpm. The motor that I used so far, has an output shaft speed of 20 rpm. I replaced it with a type that turns at 13 rpm. I.e., a speed reduction of 35%. It has exactly the same size and mouting features as the 20 rpm model, so the replacement only took a couple of minutes.

With my motorized coupling loop with 16 cm (6.3") diameter, the SWR is adjustable to 1.1 in all bands.


Make a new clear polycarbonate hood, similar to the large one that I made for my 1-turn 80-20 STL. Simple rectangular box, open at the bottom [easier than with the capa installed on the outside of the bottom of the main loop]. Plate thickness: 4 mm. Five plates: top, long side x 2, short side x 2. Plus 4 narrow 4 mm strips, same length as the inside of the 4 side plates, to support the hood onto the PPE motor drive base plate.

Hood high enough to fully cover capa + connections, even when not installed horizontally (i.e., loop rotated about 30° max), but not sticking out below the main loop.

It is made of clear, colorless polycarbonate (PC, e.g., Lexan™). This material is harder and stronger than acrylics such as plexiglass (with trade names such as Plexiglas (with one "s"), Acrylite, Lucite, Perspex). It is also easier to drill and cut than plexiglass - without breaking or cracking it. It is also available with UV protection (plexiglass is inherently more UV-resistant). On the downside: it is about 35% more expensive than same-dimensions plexiglass sheet. Another issue is bonding sections of polycarbonate. You absolutely can not use (and do not want to use) cyanoacrylate glue (a.k.a. "Super-Glue"). PC requires a special one- or two-component "glue", in general a Methyl Methacrylate Adhesive (MMA) solvent. The good stuff is toxic!, so you have to do the gluing outdoors or in a very well ventilated area! I used SCIGRIP® 16 glue. Note that some MMAs are colored when cured - not what I want! SCIGRIP 16 is still available (2021) at do-it-yourself stores and on-line shops in the US (but is not for sale in southern California) and the UK. It is on the "hazardous material" list in mainland Europe, and basically not allowed to be shipped to there (and only via surface-mail within the US).

I re-used my very simple wooden jig that I made to glue-up the polycarb plates of the motor-drive hood of my 1-turn loop.

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Fig. 32: My design for the hood

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Fig. 33: The custom-cut pieces of polycarbonate sheet - white protective film on both sides

(the two narrow strips without white film on them are cut from left over pieces of another hood)

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Fig. 34: The various pieces of the hood - all glued up

(the 30 cm / 1 ft ruler is shown as size reference)

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Fig. 35: The installed hood

The hood weighs 725 grams (≈ 1.7 lbs). This is about half the weight of the motor-capacitor assembly (1.5 kg). Total weight of my 2-turn STL is 5.9 kg (≈ 13 lbs).

Compare this to my 1-turn STL: the hood of its capacitor drive unit is more than twice as long and weighs 2.5 kg (≈ 5.5 lbs), the capacitor drive unit itself weighs 4.2 kg (≈ 9.3 lbs), including the large 2.2 kg (≈4.9 lbs) vacuum capacitor (10 kV, 500 pF). Total weight of the 1-turn STL is 12.3 kg (≈ 27 lbs) = more than twice that of the equivalent 2-turn STL.


Needed because coupling different loop position required for positioning at the middle of my terrace vs 1+ m above my steel pergola. Same type of drive as successully used with my 1-turn STL. Added same motor selection relay to the vacuum capacitor motor drive, so 100% compatible with the remote control box of that I made for my 1-turn loop.

Support for loop: made screw-and glue PVC tubing adapter.

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Fig. 36: Linear actuator with custom PVC elbow and BNC to male banana adapter

(BNC adapter attached with two cable ties)

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Fig. 37: Motor drive assembly of the vacuum capacitor - expanded with motor selection relay and DC power jack

(two 5 VDC SPST relays with solenoids in series, as in my 1-turn STL drive); power plug of the linear actuator is inserted from below)

My miniVNA measurements (with 0 dBm power, i.e., 1 mW into 50 ohms) show that the coupling loop motor drive has no discernable impact on the resonance bandwidth  ( = "Q") of the antenna, compared to a simple manually adjustable coupling loop. Also, transmission with 80-100 W shows no undesirable effects either.


Graph: resonance freq vs capa revs, in umbrella stand, on telescopic mast @ 2m and 4m above ground, telescopic mast @ 1m above pergola.

Conclusions regarding tuning range for used varicap, also compared to 1-turn loop.

Tuning range with 5-250 pF cap: INDOORS in umbrella stand, bottom of loop 1m above floor: 3.44 - 12.8 MHz, compared to the self-resonance frequency of 17.95 MHz (= without the capacitor). I.e., for the given tuning capacitor, the antenna covers the 80-40-30 m bands. To cover 20 m: make loop smaller, and use a larger capacitor (because the low end of the tuning range will also move up). --> validated my decision to go for a varicap with 250 pF max, i.e., half the max of the varicap of my 1-turn loop.

SWR= 2.618 = - 3dB = half-power bandwith: Q is about 1325 around 3590 kHz. Compare this to my 1-turn loop: BW = 4.3 kHz around 3580 kHz --> Q = 845.

TERRACE in umbrella stand, bottom of loop 1m above floor:

80-30: requires full stroke of the CL motor drive!

With the STL placed at the standard position on my terrace (see Fig. 43below), . Note that at this position, the STL "sees" a wall on two sides, and a concrete overhang and steel pergola in front. The steel rebar and the pergola beams are connected to ground/earth of my apartment's electrical system (and associated electrical noise). In the 80 m band, I could reduce the received noise level by 2 S-points (12 dB power level) by rotating the antenna over 90° from the maximum noise direction.

TX/RX directivity: like Fig. 86B on 80-20 STL page?

80m: SWR 1.1 with 34 cm diam coupling loop halfway between top & center of loop and turned 45° out of main loop plane. SWR 1.1 with 19 cm diam coupling loop coplanar with main loop, 10 cm spacing wrt main loop.

80m: SWR=2 bandwidth ≈2 kHz, vs ≈3.2 kHz for my 1-turn loop. You don't want less than that vs B/W of modulation and need to be able to very finely tune. 0KDF theoretical prediction for BW?

Effect of adding/removing hood?

Obviously, any movement of the turns with respect to each other changes the loops self-inductance, which causes a shift in the resonance frequency and SWR. So far, the loop turns are already attached at several points. The lowest point of the loop turn that is nearest the mast is already attached to the mast. The top of the two turns are attached to the "gallows". At the bottom, the ends of the loop's tubing are attached to  the vacuum capacitor "bottle". The next Figure shows a snaphot of the effect of just a smal breeze, when the movement of the loop turns is not restricted any further:

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Fig. 38: No spacers installed - effect of varying loop-turns interdistance due to a light breeze

Clearly, the movement of the loop-tuns must be limited. So I installed two spacers between the loop turns:

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Fig. 39: Adding spacers to limit movement of the loop turns

I decided to place them at the 3 and 9 o’clock position. Placing them lower would put them closer to the capacitor and the associated high voltage. However, I did not experiment with this.

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Fig. 40: Two pairs of PVC spacers - for two different coil pitches

Installing the two spacers caused no significant change in SWR or Q (at miniVNA power level), but the resonance frequency shifted 22 kHz downward. This implies an increase in the loop's self-inductance. This is not surprising when introducing a dielectric between the turns. I have not systematically checked the effect on SWR, Q, and resonance frequency during rain and fog!

???? Without the two PVC spacers between the loop turns, the resonance frequency increased about 35 kHz in the 80m band (3620 --> 3655 kHz). No signifcant difference in bandwidth.

In order to minimize the frequency shift, and any other potential effects, I minimized the amount of spacer material by drilling a hole in the spacers - vertically, to minimize water collecting in the spacer:

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Fig. 41: Making 15 mm Ø hole in each spacer increased the resonance frequency by about 1/4 kHz, but no change in "Q"


This section is what it is all about: how does this 2-turn STL compare to my 1-turn 80-20 STL (that has the same total circumference = conductor length)? First a weight-and-size overview:

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Fig. 42: My 1-turn and 2-turn loop antennas - size & weight comparison summary

So, what does this size and weight reduction cost, in terms of "performance"? I am basically only interested in DX, so performance is (relative) signal strength at receivers that are far away. For transmission tests, I monitor and measure my own signal at remote online receivers: Web-SDRs or Kiwi-SDRs. I can do that by myself 24/7, without having to make scheds with other stations.

For the best comparison results, we want the following conditions:

  • The same antenna installation environment (installation position and height above the floor or surface), and antenna orientation.
  • The same propagation conditions (avoid fluctuations such as fading effects).
  • The same frequency.
  • The same transmitter output level.

I considered two options.

  • Option 1: Install the two antennas "relatively" close to gether, but no so close that the antennas "significantly" influence each other or have a different interaction with the environment. This allows near-instantaneous switching between the antennas.
  • Option 2: test one antenna, then (quickly) replace that antenna with the second antenna at exactly the same spot, and test that one.

Assuming a wide open installation environment (i.e., no objects anywhere in the near field of the antennas, Option 1 is doable with low-Q antennas. However, it is absolutely not trivial with two high-Q antennas - such as STLs - at approximately the same frequency! Basically, the coupling factor between the two antennas should be small compared to the product of their Q. For my 1-turn and 2-turn STL, this is  ≈845 and ≈1350, respectively! This implies the need for large separation distance between the antennas, and/or large frequency difference. 

Before going through the trouble of installing my STLs at an elevated position (on top of my pergola), I tested their interaction while installed on the terrace floor, spaced 2.5 m, and oriented the same way (i.e., the loops in parallel). I selected this distance, because it would be what I would use on top of my pergola, with its 360° unobstructed view.

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Figure 44: my 1-turn and 2-turn STLs placed for the interaction test and the 2-turn STL de-tuned by jumpering

I tuned the antennas to frequencies around 3.6 MHz, and used a jumper cable across the capacitor of one of them. Without this de-tuning, the coupling becomes very clear when the difference in resonance frequencies of the two antennas is less than about 40 kHz, i..e, about 10x the half-power bandwidth: the SWR curve shows a second resonance dip. This dip moves with changes of the primary resonance frequency, and becomes smaller when the difference in resonance frequencies is increased:

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Figure 45: the SWR curve clearly shows a second resonance dip due to coupling effects

When the stand-alone resonance frequencies differ by 80 kHz, spacing the antennas by 2.5 m and jumpering one of them, causes the resonance frequency of the not-jumpered antenna to shift by about 2 kHz! For 90 kHz difference, the shift was about 1.45 kHz. Clearly, this is significant interaction - even though the SWR was not significantly impacted. It made no difference whether the coupling loop of the antenna that was not hooked up to my antenna analyzer, was terminated with a 50 ohm dummy load resistor vs. left "open". Based on these observations, I decided that I would use 2.5 m spacing (≈8 ft), and tune the STLs to resonance frequencies spaced by at least 100 kHz.

For "Option 1" transmission comparison tests, I would have placed one STL centered on top of my steel pergola, the other  2.5 m to the left, centered on the concrete overhang of my roof:

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Figure 43: The STL placement situation on my terrace

The steel pergola is grounded to the electrical system of the building. The concrete does have steel rebar in it, but represents a different "soil" to the antenna above it. Furthermore, I would be limited to a single transmission direction: the planes of the STLs would have to remain parallel and concentric. For all other pointing directions, planes of teh loops would no longer be concentric, and the distance between the loops would be smaller! This is why I decided to go with Option 2.

During the evenings of 26 and 27 April 2022 (no day-time DX on 80m), I performed a number of PRELIMINARY comparative measurements in the 40 and 80 m bands::

  • My QTH: in the south of France, QRA locator JN03qo.
  • Remote receiver: online WebSDR at Maasbree (in the south of The Netherlands), QRA locator JO31ai, distance 930 km (≈580 miles), bearing ≈20° east.
  • I always use remote online receivers, as they are available 24/7, without having to make scheds with other stations. Most Web-SDR's world-wide are here: www.websdr.org; there is also a number of Kiwi-SDRs around the world.
  • I used the same WebSDR that I use to listen to, and print, the weekly European Feld Hellschreiber net (active since the 1980s!). For my tests, I would have preferred an online remote receiver at (much) closer range. Unfortunately, in France, amateur radio and online SDRs are not as popular as in other countries, so the SDRs are few-and-far-between...
  • Local sunset: 20:50 CEST ( = UTC +2 hrs)
  • Transmitter power: adjusted to 50 W (at the SWR/Power Meter at the transmitter output). Same coax cable used for both antennas.
  • Antennas installed at the same position, with same distance beteen the bottom of the loop and the surface below (here: the top of my heavy steel pergola).
  • Antenna coupling loops adjusted for SWR < 1.1
  • Transmit intervals: 3-4 minutes constant carrier each.
  • Signal strength plots: screenshots from the live plots provided by the WebSDR; I enhanced the signal strength peak envelope with a heavy solid line, and added an eyeballed red line for the average signal strength.

The first evening, I did three series of test transmissions in the 40m band:

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Figure 46: First test series in the 40m band - my 2-turn STL

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Figure 47: Second test series in the 40m band - my 1-turn STL at the same position

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Figure 48: Third test series in the 40m band - 2-turn STL, repeat of first series, to check propagation conditions change

All plots show rapid propagation fluctuations. Preliminary conclusions for 40 m:

  • In the far field, both antennas have a fairly "round" radiation pattern - as to be expected.
  • In terms of signal strength at the remote receiver for the same transmitter power, the 2-turn STL is about one S-point (6 dB) weaker. Note: 1 S-point ≈ factor 4 in power!

The next evening, I repeated the measurement in the 80 m band. Conditions were not great, but anyway...

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Figure 49: First test series in the 80m band - my 2-turn STL

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Figure 50: Second test series in the 80m band - my 1-turn STL at the same position

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Figure 51: Third test series in the 80m band - 2-turn STL, repeat of first series, to check propagation conditions change

Preliminary conclusions for 80 m:

  • Inconclusive. Comparing the first and the second series, the 2-turn STL is about 1½ S-point (≈10 dB) weaker. Note: 10 dB ≈ factor 10 in power! Comparing the second and third series, the difference is closer to about one S-point (6 dB)

I would like to repeat the tests with a local or regional remote receiver, to reduce the impact of fading and noise uncertainty. Possibly a "receive" test with a beacon station that transmits a constant CW signal, instead of a "transmit" test with remote receiver. 


"Models are always wrong, but some are useful" (George E.P. Box, statistician, 1976)


TO BE ADDED: antenna radiation pattern simulations with the excellent 4NEC2 freeware simulation package.

Add caveats about NEC-based simulations have significant limitations regarding accounting for proximity effects of conductors. Ref. to be added.

Use the convenient "helix" shape creator in the Geometry Builder function of 4NEC2, for the basic 2-turn loop:

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Fig. 50: 4NEC2 modeling of the basic 2-turn loop

Note: in the Helix Geometry Builder, entry of values for loop length/height, loop radius, and conductor radius is in m, cm, and mm, respectively! The loop is oriented vertically and in the XZ plane by entering "90 90 0" for "Rotate X, Y, Z" in the "Helix" window. Then add the 15 cm long capa connection stubs ( = 90° bent ends of the loop tube), add capa across these stubs. Add coupling loop (also as helix?). Caveats, segment errors. In the Source/load" tab of the 4NEC2 editor, the "Show loads" box is checked and in "Load(s)" line item 1, "Wire-conduc" is selected in the "Type" column, and "Copper" is selected in the "Cond(s) column. All other column field remain blank.

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Fig. 51: 4NEC2 modeling of the complete 2-turn loop - with capacitor and coupling loop

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Fig. 52: Radiation pattern and current distribution of the modeled 2-turn loop

(capacitance zero & TBD? height above ground?, frequency?, ground type?)

Compare against similar simulation of 1-turn loop - also construct model with "Helix" builder function of 4NEC2.

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Fig. 53: 4NEC2 modeling of the basic 1-turn loop

(note the tiny gap between the ends of the loop (at the bottom of the loop) - the helix tool does not allow zero pitch "length")

Per this very detailed and comprehensive on-line coil RF-inductance calculator, this 2-turn coil - by itself - has an inductance of ≈4.1 μH (at 3.6 MHz), compared to ≈2.7 μH for the same-tube-length 1-turn coil. Due to numerous non-trivial effects, this calculated RF inductance varies with RF frequency: ≈3 μH vs. ≈2.3 μH (at 7 MHz), and ≈3.5 μH vs. ≈2.5 μH (at 10 MHz).


External links last checked: July 2021 unless noted otherwise.

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