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From a Back-to-Back Trace to a Real EFHW Transformer Test

EFHW transformer test practice

From a Back-to-Back Trace to a Real EFHW Transformer Test

Two transformers connected nose-to-nose can reveal useful small-signal behaviour. They cannot, by themselves, prove the loss of one transformer on an installed antenna.

ON6UREBack-to-back testsEFHW transformersVNAUncertainty
Related reading
Why Back-to-Back EFHW Measurements Keep Fooling People EFHW Transformer Design and Qualification Common-Mode Choke Test Jigs: Prove You Measured the DUT S21 Choke Measurements: When the Series Model Breaks

The familiar experiment is attractive: transform 50 Ω upward through one EFHW transformer, reverse the ratio through a second transformer and measure between two 50 Ω instruments. If the pair loses 0.4 dB, it is tempting to write 0.2 dB on each unit. That split is an estimate with conditions, not a universal measurement law.

Keep the conclusion inside the fixture. A back-to-back result belongs to that pair, junction, calibration, frequency, small-signal power and temperature. Extend it to one transformer or an antenna only after the missing assumptions are tested.

What the Pair Actually Measures

A full two-port VNA measurement returns S11, S21, S12 and S22 for the complete cascade between its calibrated planes. That includes both transformers, connectors, low-side wiring, the high-impedance junction, compensation components, enclosure coupling and any unintended exterior-current or radiation path.

The pair is useful for finding:

  • small-signal passband and resonances;
  • input and output mismatch;
  • forward/reverse transmission and reciprocity;
  • repeatability between builds and orientations; and
  • sensitivity to junction length, spacing, shielding and compensation.

It does not contain an installed EFHW radiator, its ground environment or its coax return path. It therefore cannot measure antenna radiation efficiency, realized gain or pattern.

Why Pair Loss Is Not Automatically Twice Unit Loss

If two electrically identical, reciprocal units are cascaded with a well-defined internal connection and negligible fixture effects, half the pair loss in decibels can be a useful estimate. Real high-ratio transformers challenge each assumption.

The high-impedance ports are sensitive to lead inductance, a few picofarads of capacitance, enclosure position and nearby conductors. Their complex port impedances may not be conjugately matched at the junction. Waves can reflect repeatedly between the two units, and the phase of that interaction can raise or lower S21.

Reciprocal is not the same as symmetric. A passive transformer may have equal forward and reverse transmission while its low- and high-impedance ports have different reflection coefficients. Reversing a ratio does not cancel every parasitic.

Make the Bench Result Reproducible

Before comparing traces, record:

  • transformer topology, winding arrangement and component values;
  • port definitions, reference impedance and calibration planes;
  • high-impedance-junction length, spacing, support and shield geometry;
  • cable and adapter characterization or de-embedding method;
  • sweep power, IF bandwidth, averaging and frequency points;
  • orientation of cores, enclosures and coax; and
  • temperature, unit identity and connector repeatability.

Repeat the measurement with the two units exchanged and each physically reversed where the topology allows it. A result that moves with orientation or spacing is evidence that the fixture is part of the measurement.

Use All Four S-Parameters

S21 magnitude alone hides input mismatch, output mismatch and phase. Measure S11, S21, S12 and S22 as complex quantities. If the units and junction can be represented by characterized two-port networks, cascade or de-embed them with scattering-transfer methods rather than multiplying magnitudes alone.

Calibration removes systematic error only to its stated planes. Port extension corrects electrical delay; it does not generally remove connector, launch, lead and high-impedance-junction behaviour.

Add a Representative Load Matrix

An EFHW feedpoint is a complex, installation-dependent load. A nominal 49:1 calculation maps one 2450 Ω resistance to 50 Ω in an ideal transformer, but the antenna rarely presents that fixed value across all used bands.

After the pair test, evaluate a single transformer with characterized loads spanning the resistance and reactance expected at its antenna port. For each load, record input impedance, accepted power, delivered power, fixture loss and uncertainty. Do not expose an ordinary resistor or VNA fixture to voltage beyond its rating.

Test stage What it supports What remains unknown
Back-to-back VNA sweep Composite small-signal S-parameters of pair and fixture Unique per-unit loss, power behaviour and antenna efficiency
Swap/reverse and spacing trials Repeatability, reciprocity and fixture sensitivity Installed complex-load performance
Single unit with load matrix Match and delivered power versus representative loads High-power thermal and insulation margin
Rated-power thermal test Loss, drift and temperature for stated waveform and duty cycle Antenna pattern and radiation efficiency
Installed current/pattern test Return-path current and antenna-system behaviour at that site Universal performance at another installation

Small-Signal Loss Is Not Rated-Power Loss

A VNA normally operates at milliwatt levels. At transmitter power, ferrite behaviour, conductor resistance, dielectric loss and temperature may change. Reactive loads can create high winding current or terminal voltage even when average delivered power seems modest.

A rated-power test needs calibrated incident, reflected and delivered-power planes, a characterized load, remote temperature sensing, a declared waveform and duty cycle, safe clearances and an uncertainty budget. Do not infer continuous-duty capability from a brief speech-peak test.

Turn the Test Into a Power Ledger

Report the quantities separately:

  • incident and reflected power at the transformer input;
  • power accepted by the transformer;
  • power delivered to the characterized load;
  • fixture and connector loss;
  • transformer temperature rise and stabilization time; and
  • measurement uncertainty.

If a result is only the pair’s S21, publish it as the pair’s S21. That is not a weak conclusion. It is an honest and repeatable starting point for the next experiment.

Engineering References

  • Keysight: S-Parameter Techniques for Network Design
  • Keysight: De-Embedding and Embedding S-Parameter Networks
  • NIST: De-Embedding and Unterminating Microwave Fixtures
  • Fair-Rite: Use of Ferrites in Broadband Transformers

Follow the Current Path, Not the Folklore

Explore more RF.Guru technical deep dives on transmission lines, common-mode current, baluns, chokes and antenna measurement—and subscribe for new engineering articles and laboratory notes.

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Mini-FAQ

  • Is a back-to-back transformer test useless? No. It measures the composite small-signal network of the pair and included fixture under declared conditions.
  • May I divide the pair loss by two? Only as a bounded estimate after showing that the units are equivalent and the junction, mismatch, fixture and uncertainty support that split.
  • Why measure all four S-parameters? S11 and S22 reveal port mismatch, while complex S21 and S12 show transmission, phase and reciprocity.
  • Does calibration remove the high-impedance junction? Only if the calibration or validated de-embedding explicitly moves the reference planes past it.
  • Can a VNA certify high-power transformer efficiency? No. It characterizes the small-signal state; operating-power loss and heating require a rated test.
  • Does the pair result prove EFHW radiation efficiency? No. The installed radiator, ground, return path and radiated power are outside the fixture.

Questions, antenna-factor records or height trials to share? Contact RF.Guru.

Joeri Van Dooren, ON6URE — RF engineer, antenna designer and founder of RF.Guru, specialising in practical HF/VHF receiving systems and RF components.

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