Magnetic Loop Antenna Selfmade 3P HB9BPO

Info: Mag loop made of copper tubing with an air variable capacitor.
Conductor: Copper tube OD 12 mm, ID 10 mm, bare surface.
Capacitor: Air variable capacitor, self-made, CNC-milled from aluminum sheet.
Environment: In the garden, on a Styrofoam box on a wooden table. Center loop 1.40 m above ground.
Thanks: Many thanks to Peter HB9BPO for the support, the fun conversations, and the catering.

Antenna Efficiency Overview

Band 20m 17m 15m 12m 10m
Frequency f MHz 14.072 18.116 21.253 24.947 28.604
Intrinsic bandwidth Bint kHz 99.1 102.7 123.6 165.6 201.9
Source of Bint S-Parameters
Loop diameter D m 0.762
Conductor diameter d m 0.012
Loop count n 1 1
Inductance L H 2.02e-06
Capacitance C pF 63.2 38.1 27.7 20.1 15.3
Unloaded Q0 1 142 176 172 151 142
Damping resistance RT Ohm 1.261 1.306 1.572 2.107 2.568
Radiation resistance RR Ohm 0.0316 0.0872 0.166 0.316 0.550
Loss resistance RLoss Ohm 1.229 1.219 1.406 1.790 2.018
Power to antenna Pfwd W 10 10 10 10 10
swr_min 1 1.39 1.04 1.03 1.08 1.11
etaSWR_ant % 97.4 100.0 100.0 99.9 99.7
Power antenna load Pload W 10 10 10 10 10
Antenna efficiency η % 2.44 6.67 10.5 15.0 21.4
Loop current I rms A 2.78 2.77 2.52 2.18 1.97
Loop voltage Uloop rms V 497 637 682 691 717
Magnetic dipole moment m A m² 1.266 1.260 1.149 0.992 0.898
Link to calculator calculator calculator calculator calculator calculator

Build Details

Homemade magnetic loop made from copper tube. A common-mode choke is clearly visible on the vertical cable.
At the top is a coupling loop made from brass tubing (loop diameter: 170 mm, tube diameter: 6 mm).
The coupling loop is fixed only with adhesive tape. The SWR was very good with exactly this setting, and the position was kept unchanged for all measurements.
Air-variable tuning capacitor with hand knob and stepper motor drive (black stepper motor in the rear).
Detail view of the loop construction and mounting hardware.
Homemade tuning capacitor, CNC-milled on a self-built milling machine from aluminum sheet.
For lower bands, additional capacitors can be switched in.
The switch was open for all measurements shown here, so it was not used.
The connection to the copper tube is made using screwed ring lugs and copper wires.

With the variable capacitor, the frequency can be tuned from 13.41 MHz up to 29.78 MHz.
The capacitor has external dimensions of approximately 40 mm x 40 mm x 220 mm.

Environment

The antenna stands on a wooden table in the garden. A styrofoam box was used to increase the ground clearance a bit more.

The loop center is 1.40 m above ground.
The nearest object in the surroundings is a clothesline post at a distance of about 2.5 m (visible on the left in the picture).
The grass is dry.

Measurement Info

The antenna measurement setup is very practical. We sit at a table about 5 m away from the antenna.
A 10 m long LMR195 cable runs from the antenna to NanoVNA V2 Plus4.
Here we can also switch over to IC-7300 MK2 as transmitter.
For tuning, we measure the resonance with the VNA, and the capacitor is adjusted with a stepper motor.

VNA measurements

The antenna S11 parameters were measured with the NanoVNA V2 Plus4.
The following values were derived from these measurements.
Details on the measurement method can be found here.

VNA calibration: fusspunkt_vna.svg
The calibration of the VNA was done at the antenna feed point: green line.
Common-mode choke at the antenna: positron.ch/rf/choke_simple
Used cables: 80 cm RG400 (including the choke) and 10 m LMR195.
The cable attenuation alpha and the cable delay tau in the following table should therefore be small.

File model f0
MHz
model BSWR2_62
kHz
model alpha
db
model_tau
ns
SWR min eta SWR
20260827_1344_antenne_14p1MHz_VALUES.py 14.072 99.1 0.000 6.24 1.39 0.974
20260827_1409_antenne_28p6MHz_VALUES.py 28.604 201.9 0.000 4.96 1.11 0.997
20260827_1419_antenne_24p9MHz_VALUES.py 24.947 165.6 0.000 5.22 1.08 0.999
20260827_1426_antenne_21p3MHz_VALUES.py 21.253 123.6 0.000 5.73 1.03 1.000
20260827_1435_antenne_18p1MHz_VALUES.py 18.116 102.7 0.007 6.01 1.04 1.000

The following diagrams: red points = measured values; green line = fitted model.

Smith SWR Values

20260827_1344_antenne_14p1MHz

20260827_1344_antenne_14p1MHz smith

20260827_1344_antenne_14p1MHz

20260827_1344_antenne_14p1MHz swr

20260827_1344_antenne_14p1MHz

model_f014.072MHz
model_BSWR2_6299.1kHz
model_alpha0.000db
model_tau6.24ns
SWR_min1.39
eta_SWR_ant0.974

20260827_1409_antenne_28p6MHz

20260827_1409_antenne_28p6MHz smith

20260827_1409_antenne_28p6MHz

20260827_1409_antenne_28p6MHz swr

20260827_1409_antenne_28p6MHz

model_f028.604MHz
model_BSWR2_62201.9kHz
model_alpha0.000db
model_tau4.96ns
SWR_min1.11
eta_SWR_ant0.997

20260827_1419_antenne_24p9MHz

20260827_1419_antenne_24p9MHz smith

20260827_1419_antenne_24p9MHz

20260827_1419_antenne_24p9MHz swr

20260827_1419_antenne_24p9MHz

model_f024.947MHz
model_BSWR2_62165.6kHz
model_alpha0.000db
model_tau5.22ns
SWR_min1.08
eta_SWR_ant0.999

20260827_1426_antenne_21p3MHz

20260827_1426_antenne_21p3MHz smith

20260827_1426_antenne_21p3MHz

20260827_1426_antenne_21p3MHz swr

20260827_1426_antenne_21p3MHz

model_f021.253MHz
model_BSWR2_62123.6kHz
model_alpha0.000db
model_tau5.73ns
SWR_min1.03
eta_SWR_ant1.000

20260827_1435_antenne_18p1MHz

20260827_1435_antenne_18p1MHz smith

20260827_1435_antenne_18p1MHz

20260827_1435_antenne_18p1MHz swr

20260827_1435_antenne_18p1MHz

model_f018.116MHz
model_BSWR2_62102.7kHz
model_alpha0.007db
model_tau6.01ns
SWR_min1.04
eta_SWR_ant1.000

Inductance

The main loop inductance is an important parameter because it directly affects the antenna efficiency calculation.
The inductance can be estimated from geometry (L). In general, an additional measurement is used as a cross-check, especially for non-circular loops where the geometric estimate is more difficult.

Inductance cross-check measurement

The resonance frequency of the LC circuit depends on L and C. Additional known capacitors are connected in parallel with the existing capacitor, and the new resonance frequency is measured.

Capacitor switching concept
Schematic of the switched capacitors
Inductivity picture: 20260827_115219934_cap_switch.jpg
The switched capacitor is visible in the picture above.
The connections were temporarily taped to the main loop with yellow tape.
With two switches (only one is visible in the picture because they are exactly behind each other), the two capacitors can be switched in.

fNIX18.112769MHzResonance frequency with no additional capacitors connected.
fOFF17.296894MHzCapacitors and switches are physically connected at the antenna capacitor.
A small parasitic capacitance from wiring and switches lowers the resonance frequency.
f1009.369003MHzResonance frequency with an additional 100 pF capacitor switched in.
f5604.450705MHzResonance frequency with an additional 560 pF capacitor switched in.
C100100.0pFAdditional capacitance used for the 100 pF branch.
C560579.0pFAdditional capacitance used for the 560 pF branch.
L2.024e-06HCalculated from geometry of the main loop.
L1002.039e-06HDerived from the resonance frequencies fOFF and f100
deviation +1% vs L
L5602.062e-06HDerived from the resonance frequencies fOFF and f560
deviation +2% vs L
CNIX3.656e-12As/VDerived from using L100, fOFF, and fNIX
estimated parasitic capacitance of switches and wiring; expected value 1 ... 5 pF

The maximum deviation between L and the capacitor-based L1x values is +2%. This is considered a small deviation and is accepted. L is used for the calculations of the antenna efficiency.

Cross-check H-field

The H-field can be calculated under free-space conditions. In practice, however, the building contains numerous conductive objects that distort the field. To quantify the extent of this distortion, the H-field was measured and compared with the theoretical predictions.

The H-field is measured with a small measurement loop. The measuring setup is described in https://arxiv.org/abs/2607.10828.

A was used as the transmitter: 10 W, FM.

View to the south.
HB9ISP Peter taking measurements.
The measurement loop is at the same height as the antenna and above the measuring tape lying on the ground.
Antenna in the garden.

Even small deviations in position cause large changes in the measured value, because points A and C are very close to the antenna and the field therefore changes rapidly.
At positions A and B, the field lines run exactly as expected from the theoretical free-space field-line pattern. At position C, the field lines are tilted slightly upward (orientation of the measurement loop at maximum measured value).

f = 14.072 MHz

tx_power_w10.0
f_Hz14072000
attenuation_cables_connectors_total_dbm0.76 dB
tx_after_cable_w8.4
I_main_loop_A2.5
magnetic dipole moment m (Am2)1.2
XYZexpectedmeasuredfactor
mmmA/mA/m
A 0.0 2.0 0.0 0.0113 0.0089 0.790
B 0.0 7.0 0.0 0.0010 0.0031 3.019
C -2.0 0.0 0.0 0.0237 0.0246 1.039

f = 18.116 MHz

tx_power_w10.0
f_Hz18116000
attenuation_cables_connectors_total_dbm0.83 dB
tx_after_cable_w8.3
I_main_loop_A2.5
magnetic dipole moment m (Am2)1.1
XYZexpectedmeasuredfactor
mmmA/mA/m
A 0.0 2.0 0.0 0.0104 0.0120 1.145
B 0.0 7.0 0.0 0.0018 0.0033 1.851
C -2.0 0.0 0.0 0.0267 0.0177 0.663

f = 21.253 MHz

tx_power_w10.0
f_Hz21253000
attenuation_cables_connectors_total_dbm0.89 dB
tx_after_cable_w8.2
I_main_loop_A2.3
magnetic dipole moment m (Am2)1.0
XYZexpectedmeasuredfactor
mmmA/mA/m
A 0.0 2.0 0.0 0.0095 0.0177 1.862
B 0.0 7.0 0.0 0.0022 0.0031 1.398
C -2.0 0.0 0.0 0.0271 0.0173 0.639

f = 24.947 MHz

tx_power_w10.0
f_Hz24947000
attenuation_cables_connectors_total_dbm0.95 dB
tx_after_cable_w8.0
I_main_loop_A2.0
magnetic dipole moment m (Am2)0.9
XYZexpectedmeasuredfactor
mmmA/mA/m
A 0.0 2.0 0.0 0.0093 0.0180 1.937
B 0.0 7.0 0.0 0.0027 0.0039 1.459
C -2.0 0.0 0.0 0.0256 0.0155 0.605

f = 28.604 MHz

tx_power_w10.0
f_Hz28604000
attenuation_cables_connectors_total_dbm1.00 dB
tx_after_cable_w7.9
I_main_loop_A1.8
magnetic dipole moment m (Am2)0.8
XYZexpectedmeasuredfactor
mmmA/mA/m
A 0.0 2.0 0.0 0.0102 0.0132 1.303
B 0.0 7.0 0.0 0.0032 0.0058 1.816
C -2.0 0.0 0.0 0.0249 0.0205 0.825

The measured field matches the free-space prediction reasonably well.
The largest deviations occur at point B.

Final Remarks

This homebrew magnetic loop is a very nice DIY build.

It is lightweight, simple, and easy to transport.
The self-made capacitor with CNC-milled plates looks excellent and works flawlessly.
The coupling loop was already nearly perfectly matched from the start and was kept unchanged for all measurements.
The efficiency is not outstanding, but for the small loop diameter and simple construction it is appropriate.
There are probably many similar homebrew antennas around the world.


Overview of all Antennas with filter/selection: compare page
Overview of all Antennas static: static compare page
2026 Peter Märki (HB9ISP). This project is created in my free time and has no commercial background. Provided without warranty of any kind. Feedback is welcome.