a magloop in rough weather
Building a small transmitting loop (Magnetic Loop)

Junk box loops are do-able certainly, but need just that bit more attention to the quality of connections if they are to be effective radiators. The essential point to remember is that the radiation resistance of a magloop is very low.

Radiation Resistance (Rr)

Rr is a concept rather than something real - whereas when you feed energy into an antenna, some of it is lost as heat across the actual resistance of the antenna, the energy that is radiated is said to have been dissipated across the radiation resistance.

Clearly if Rr is low, then the actual resistance must be kept very low indeed so that it does not dissipate most of the input power as heat. Use single pieces of conductor with as few joints as possible, and the largest diameter hollow conductor practical to minimise losses (hollow because that saves weight and cost, and the RF only travels just below the skin of the conductor anyway).

Calculating your loop size

The calculations can be done with pen and paper, a calculator, or increasingly with computer spreadsheets and dedicated programs. The calculations that you need concern the diameter of the main conductor, the capacitance and voltage rating of the tuning capacitor and the size and position of the inductive feed loop - unless you are tapping the feeder directly onto the loop. Efficiency and bandwidth are often revealed too.


'Q' or the measure of 'goodness' of a tuned circuit is one of the more tricky parts of the calculation. It is best measured with the completed antenna in place rather than calculated because it is so dependent on surroundings such as feed point and proximity to earth.

Reg G4FGQ has written a number of loop design programs that are freeware and available for download here, but some of the formulae used are detailed here

formulae for loop design

For those of you who want to write your own programs, perhaps for the smaller and older computers available there is a BASIC listing that is easily converted to most dialects.

A Spreadsheet Model

If you want to model the efficiency, radiation resistance, capacitor voltages and sizes of an example magnetic loop (actually built in copper) the following early version Lotus 123 compatible spreadsheet gives you 'ball-park' figures that are really quite enlightening.

boxLotus123 Loop calculations- click to download ( 6.5k )

boxExcel97 Loop calculations- click to download ( 28k! )

Some STL examples.

By way of example, I have an 180cm diameter loop for 80-30metres mounted about fifteen centimetres from the ground, against a brick wall - with a tree on the other side of it a mere thirty metres from the shack.

A smaller (80cm) loop covers 20-10metres and is mounted on an aluminium stub about a metre above a flat roof which is itself much lower than the surrounding buildings.

A have a similarly sized 80cm loop for 50MHz too, the loop is made from narrow bore copper pipe (the sort used for central heating installations) which bends easily - and has a 10pF variable air spaced variable capacitor that stays on about 50.140MHz and gives a bandwidth of about +/- 60kHz which is very usable on CW and SSB. 7pF tunes around 50Mhz and the same loop tunes down to 4m at a capacitance of about 2 pF.

A loop schematic

Drawn on a Psion series 3a palmtop using VECTOR bydiagram of 50MHz loop nick@kizzyco.com http://www.kizzyco.com/)

The 50MHz loop built from narrow bore easily bent 10mm diameter copper tubing - comes in a coil already! The loop is fastened to a 20mm diameter conduit pipe made of a sturdy plastic. The loop is attached at the upper edge (open ends) and on its lower edge using the same clips that normally run it along the skirting board.

If you motorise the tuning capacitor -which is necessary if you using the loop on anything but a spot frequency - although the bandwidth is around a 100kHz on 6m - the control line which carries the power to the motor should run down the midpoint of the main loop, so as to minimise eddy currents being induced in it.

6m mobile loop

For portable or mobile work a small aluminium stub on the car rack accepts the 20mm diameter plastic conduit that supports the loop tuning capacitor and (at the lower end) the coax feed loop.

6m mobile close up

During a sunny spell I sat in the garden and worked a station in Finland with the loop on a 12ft glass fibre mast purchased from a radio rally- seen here co-mounted with a 2m HB9CV. The non-VHF nature of this QTH is detailed elsewhere and this was just before 50MHz opened up for the summer....so it felt better than it sounds..

6m loop and 2m HB9CV

Motor Drives

The Capco/AAA commerical loops us a BBQ spit motor and gearing together with a more conventional reduction drive. I had cause to replace on of the drive units in my 80-40m loop (perhaps because I mounted it at an angle - not vertical - Im wondering if the weight of the capacitor secured as it is at one end, caused it be harder to turn and damage first the drive gears and finally the motor.

Here is a view of the disassembled gearing.

maggear1.jpg - 5713 Bytes

A close up of the gears

maggear2.jpg - 5756 Bytes

And finally a very close up of the damaged gear - notice that the teeth have been worn down uniformly all round the top of the cog - this was no sudden jam and shear failure -but wear and tear. Perhaps a lubrication issue (metal on metal?)

maggear3.jpg - 7660 Bytes

Positioning an STL

Amateurs have never followed rules! As high as possible and as far away from anything else as possible is a nice, but often unrealistic ideal. STLs do not like being near any conductors, because the magnetic flux is drawn to them, and induces wasteful currents that in turn produce unhelpful heat. The centre conductor that might support your loop is no exception, but so long as it is exactly central, the induced currents largely cancel out. Current will flow on the braid of the feeder if the STL (and feeder when nearby) is not symmetrical about it's capacitor for the same reason. The radiating ability of the antenna correlates with the area within the tuned loop - and since for a given length of conductor, a circle produces the biggest area AND circles can be free from lossy joints - you will less often see square STLs - although they exist.

Magnetic fields decay with distance faster than electrical fields- although at about 1/6 of a wavelength from the loop they are about equal intensity. However closer up, they are more penetrative.

STLs may therefore be more tolerant of unavoidable low level mounting than wire antennas, but by the same token, a small elevation of an STL can have a significant benefit.


The need to accurately tune the loop means that some form of gearing drive is needed on the capacitor. At least a ten to one step down is needed, 100 to 1 being more practical. I have only ever seen DC motors controlled by variable voltage DC supplies - this takes advantage of the high torque that an electric motor delivers, but for better control - pulsing a higher voltage and controlling the tuning rate by varying the pulse frequency would give better control - I just haven't got around to it.

Control Box for the AA&A Loop

I have been asked how the control box works for the CapCo /AA&A antennas that are still quite available second hand. This page outlines how the control box was set up.

Standing Wave Ratio

Magnetic loops are fed with unbalanced co-axial feeder. Until the main capacitor is tuned to the correct transmit frequency the antenna will not resonate, and cannot be loaded properly. Once tuned however, the smaller loop used to load the antenna then needs to be positioned to effect a 50 ohm (or 75?) match with the coaxial cable being used. Any mismatch here will result in standing waves on the coaxial cable, which in turn will radiate and reduce one of the advantages of a magnetic loop - its narrow bandpass filter effect.
Happily, once you have a loop tuned, and then position the inductive driver loop to get a 50ohm match, you can retune the transmitter and main loop without having to worry about altering the loading loop - the 50ohm match works for all resonant frequencies without further adjustment.

Feeding the loop

How to get the RF into the antenna? There are three potential ways. All the pictures on this site show the usual method which involves terminating the feeder co-axial cable with a loop round to the braid. This loop inductively couples with the larger tuned loop -using air as a dialectric. It has been customary to partially screen this loop by stripping the braid only half way around it and joining braid to central conductor at the top of the loop- leaving half the small loop as a single conductor to join the braid of the feeder. Some people feel that this offers better screening from electrostatic noise, others do it simply to make the smaller loop that bit stronger.

The second method involves directly tapping the braid of the feeder coax to ther main loop exactly opposite the capacitor. This is to keep the braid as electrically neutral as possible. The centre conductor is then tapped onto the big loop to one side of the braid connection point - adjusting for a 50 ohm match once the main coil is resonant on the transmit frequency. It isn't that easy to get a good connection with copper pipe however. The third method is to use a split capacitor, and whereas the method above taps onto the inductive part of the tuned loop, you can potentially tap onto the capacitor. It is however very complex to do, and more of a theoretical idea, than a practical one.

Email GW0TQM
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Carl GW0TQM's Magnetic loop page
Contributions comments and STL links welcomed.

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