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A 51 m End-Fed Wire on 160 m: A Deployable Compromise

An ON6URE installed-system guide

A 51 m End-Fed Wire on 160 m: A Deployable Compromise

Sometimes the available antenna is 51 metres of wire, one useful support and a short operating window. Put it up if it gets you on top band—but do not let a convenient length make claims that the installed system has not earned.

ON6URE160 mEnd-fed wireMatchingReturn pathPattern
Related reading
9:1 Long Wire vs EFHW and OCF Systems End-Fed Return Paths, Counterpoises and Common Mode Remote Antenna-Tuner Placement, Feedline Loss and Stress Resonance, Match, SWR and Efficiency Antenna Height, Ground Loss and Pattern The Phantom Third Conductor

I use EFLW51 here only as shorthand for a 51 m end-fed long wire. It is not a promise of resonance, a guaranteed tuner load or a fixed radiation pattern. It is a deployable piece of wire whose result depends on every conductor and network connected to it.

My practical position: 51 m can be a useful compromise when that is the wire and support geometry available. Treat the radiator, return path, transformer, tuner, choke and feedline as one antenna system, then decide from measurements whether it meets the operating goal.

Fifty-One Metres Is a Length, Not a Resonance

The free-space wavelength is a useful first reference:

λ = c / f, where the defined speed of light c = 299,792,458 m/s.

Dividing 51 m by that wavelength shows how rapidly the same wire changes electrical length across HF:

Example frequency Free-space wavelength 51 m expressed in wavelengths
1.9 MHz about 158 m about 0.32 λ
3.6 MHz about 83 m about 0.61 λ
7.1 MHz about 42 m about 1.21 λ
14.2 MHz about 21 m about 2.42 λ
28.4 MHz about 10.6 m about 4.83 λ

Across the 1.8–2.0 MHz amateur band, 51 m is roughly 0.31–0.34 λ in free space. It is neither a free-space quarter wave nor a half wave. The complete installation may present a resistance-dominated impedance somewhere in or near the band, but that is not something the tape measure can guarantee.

Wire diameter, insulation, slope, bends, height, nearby conductors, soil and the return structure all change current distribution and feedpoint impedance. A transformer or tuner can change the impedance seen by the transmitter; it does not change 51 m into a resonant radiator.

The Other Terminal Is Part of the Antenna

An end-fed wire is not a one-terminal device. Current leaving the wire terminal is accompanied by current on the other side of the feed system. The antenna-side return can include a deliberate counterpoise or radial system, a controlled section of coax exterior, a metal support, station wiring and distributed capacitance to earth and surrounding objects.

If the coax exterior is intended to carry some of that current, its length and route belong in the antenna drawing. The common-mode choke then defines a current boundary after that deliberate section. If no boundary is established, the feedline, tuner chassis, station bonds and connected cables can become an uncontrolled part of the antenna.

A ground rod still has important protective-bonding and lightning-system duties. It is not automatically a low-impedance RF return across 160 m, and it should not be credited with that job without measurement.

Transformer, Tuner and Choke Answer Different Questions

Component What it does What it does not establish
Impedance transformer Changes the impedance relationship between its ports That a 9:1 nominal ratio is correct for the installed complex load, or that loss and stress are acceptable
Antenna tuner Transforms impedance at its own reference plane That the wire is resonant, the feedline is lightly loaded or accepted power is efficiently radiated
Common-mode choke Presents impedance to unwanted current on a transmission-line exterior That the antenna side has a sufficient intentional return conductor

A nominal 9:1 UNUN is a possible starting tool, not an automatic recipe. A lossless ideal transformer would scale impedance by the square of its turns ratio. The installed load is complex and frequency-dependent, while a real transformer adds finite magnetising impedance, leakage, capacitance, winding resistance and core loss. The tuner then has to transform whatever arrives at its plane.

Putting a suitable remote coupler at the feedpoint can keep the coax on its transmitter side closer to its design impedance. A shack tuner can make the transmitter happy while leaving substantial standing waves on the feedline between tuner and antenna. Neither architecture is universally best: tuner range, network current and voltage, feedline attenuation, weather exposure and common-mode control all belong in the decision.

A Low SWR Is Only One Reading

Matching does not itself consume the reflected power, but real feedline and networks under standing-wave conditions dissipate power. The accepted-power ledger should include conductor loss in the wire, return-path and ground loss, transformer loss, tuner loss, feedline loss and choke loss. A convenient input resistance or broad SWR dip can include loss and therefore cannot reveal radiation efficiency by itself.

Always declare the reference plane. SWR at the transceiver, impedance at the tuner input and impedance at the antenna feedpoint are different observations when lossy line or a matching network lies between them. Compare systems using the same accepted-power plane, not merely the same transmitter indication.

Higher Bands Change the Pattern, Not the Verdict

As frequency rises, the 51 m wire becomes several wavelengths long. Additional current maxima and minima can produce more lobes and deeper nulls. Whether those lobes help or hurt depends on wire orientation, slope and folds; height expressed in wavelengths; ground conductivity and terrain; the return conductor; nearby metal; and the desired propagation path.

That makes the antenna less predictable from length alone, not automatically less efficient or less useful. A particular installation may produce a valuable lobe on one upper-HF path and a null on another. Another installation using the same 51 m may behave differently. The in-force ITU-R HF pattern methodology likewise treats ground and the real environment as part of practical antenna-pattern calculation and verification.

Low physical height also needs a measured boundary. Height in wavelengths changes across the bands, so a wire that is electrically low on 160 m may be much higher on 20 m. Its elevation pattern cannot be reduced to one permanent “take-off angle.”

When the Compromise Makes Sense

A 51 m end-fed wire earns its place when the support geometry fits the site, the matching network reaches the measured load without excessive loss or stress, the return path is deliberate, unwanted common-mode current is controlled, and the installed pattern serves the intended contacts. Those are achievable engineering conditions; none follows from the number 51 alone.

It can be an especially practical way to put a substantial conductor in the air when a full-size, purpose-shaped 160 m antenna is not available. That is the useful narrative: a real, deployable compromise that can be measured and improved—not a universal top-band solution and not an antenna to dismiss because its geometry is imperfect.

Measure the Complete Installation

  • Record the geometry. Measure the wire, height profile, slopes, bends, feedpoint, return conductors, coax route, mast, station bonds and nearby metal.
  • Sweep at declared planes. Save complex impedance at the antenna side where safely accessible, at the transformer or tuner ports, and at the shack end.
  • Check the network under load. Use low power first, then monitor transformer and tuner heating, arcing margin, current, voltage and tuning repeatability at the intended duty cycle.
  • Map common-mode current. Use a characterised clamp-on RF current probe along the coax exterior, support and bonds on every intended band.
  • Account for feedline loss. Measure or calculate line attenuation for the actual load rather than applying only the matched-line data-sheet figure.
  • Model what is installed. Include height, slope, folds, return conductor, feedline section and representative ground instead of modelling an isolated straight wire in free space.
  • Verify the useful pattern. Compare repeatable field-strength or receive results with the same accepted power, rapid switching or an A/B/A sequence that restores the baseline.

My Practical Conclusion

I will gladly use 51 m of end-fed wire when it is the practical way onto 160 m. I will not call it near-resonant, easy to match, lossy, low-angle or poor on the higher bands until the complete installation supplies the evidence.

Define the return path, select the transformer and tuner from measured loads, place the choke deliberately, keep the feedline in the loss budget and verify the pattern that matters. Then the EFLW51 becomes what a good compromise should be: understandable, repeatable and honest about its boundaries.

Primary Engineering References

  • NIST Special Publication 330, Section 2 — the defined value of the speed of light used for the free-space wavelength calculation.
  • ITU-R Recommendation BS.705-2 — current HF transmitting-antenna pattern definitions and calculation guidance, including ground and environmental effects.
  • Lawrence Livermore National Laboratory: NEC—Numerical Electromagnetics Code, Method of Moments — the wire-and-ground modelling foundation and its scope.
  • Icom AH-6 automatic antenna tuner documentation — a current manufacturer example showing that supported wire length, grounding and achievable tuning remain conditional on installation and environment.
  • ARRL End-Fed Half-Wave Antenna Kit — a physical end-fed implementation with an explicit counterpoise connection.

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 51 m near-resonant on 160 m? Not inherently. It is roughly 0.31–0.34 free-space wavelengths across 1.8–2.0 MHz. Resonance and feedpoint impedance belong to the complete installed wire, return path and environment.
  • Will a 9:1 UNUN make a 51 m wire easy to tune? There is no guarantee. Nine-to-one is a nominal ideal impedance ratio, while the installed load is complex and frequency-dependent. The transformer and tuner must be selected and checked against measured loads.
  • Does a low SWR prove that the antenna is efficient? No. SWR describes impedance at a declared plane. Conductor, ground, transformer, tuner, feedline and choke loss can all reduce the fraction of accepted power that reaches the far field.
  • What is the return path for an end-fed wire? It may include a deliberate counterpoise or radials, a controlled coax-exterior section, mounting metal and distributed capacitance. If it is not intentional, connected station conductors can become part of the antenna.
  • Is a 51 m wire automatically worse on the higher HF bands? No. It becomes several wavelengths long and can develop additional lobes and nulls, but useful pattern and efficiency depend on the installed geometry, environment, return path and losses.
  • Where should the tuner and choke go? Place the tuner where it controls the intended impedance reference plane and the choke where it defines the intended common-mode boundary. Confirm both positions by load, loss and exterior-current measurements.

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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