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NEW - 4kW Inverted L Endfed Halfwave Mono Band for 40M

NEW - Carbon fibre whips for 4M 6M 10M and 20M band!

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Why EFHW Antennas Are Inherently Unstable – Especially on Low Bands

Related reading:
Why coax length before the choke matters for EFHW antennas
Why inverted-L antennas shine on the top bands

Why Flat-Top and Sloper EFHW Antennas Can Be “Unstable” on 160 m to 80 m

End-Fed Half-Wave (EFHW) antennas have gained popularity due to their simplicity and multiband (harmonic) capability. But one critical issue is often overlooked or misunderstood: the EFHW’s high feedpoint impedance makes it inherently sensitive to its environment, particularly on the lower HF bands (160 m–80 m) when using a 49:1 or 64:1 transformer.

(Scope note: this article focuses on flat-tops and slopers. Inverted-L EFHW systems behave differently and can be noticeably more repeatable on the low bands, for reasons explained below.)

The Problem with High-Impedance Feedpoints

A typical flat-top or sloper EFHW presents a feedpoint impedance often in the 2.5 kΩ–5 kΩ range (and it can move around depending on height, end conditions, and nearby capacitance). Unlike low-impedance antennas (such as center-fed dipoles), these high-Z points are very sensitive to changes in the near-field environment:

  • Humidity
  • Soil conductivity (and moisture)
  • Nearby objects (fences, trees, wet structures, gutters)
  • Rain or morning dew

These conditions alter the capacitive and dielectric environment around the antenna end and feedpoint. As a result, an EFHW that measures around 3.3 kΩ on a dry morning might drift toward 2.7 kΩ later in the day, or shift further during rain or heavy dew. Those changes can move SWR, change how “happy” the transformer is, and (most importantly) change how much the system tries to use the coax shield as a return path.

Why This Is Worse on 160 m and 80 m

On 160 m and 80 m, the antenna is electrically “large” in terms of stored reactive energy at the high-voltage end, but your surroundings are still very close in terms of the near field. Small capacitance changes (wet bark, wet leaves, a damp roof edge, a fence line) can have a surprisingly large effect because the feedpoint is sitting at a voltage maximum and the system has to “close the loop” somehow.

Reality check: a high-impedance end feed is not “wrong”... it’s just touchy. If the return path is undefined, the antenna will opportunistically use whatever it can: coax shield, shack wiring, gutters, or that one mysterious metal thing you forgot existed.

Why Inverted-L EFHW Variants Are Often More Stable

We do have inverted-L EFHW versions (using 68:1 and 70:1 impedance-ratio transformers) that tend to be more stable on the low bands... and it’s not magic. It’s geometry and physics:

  • The vertical section provides a more consistent capacitive relationship to ground and nearby terrain, which helps define the “other side” of the feed system.
  • The horizontal top loading shifts current distribution and reduces the degree to which the feed system depends on random stray capacitances at the end.
  • In practical installs, an inverted-L’s vertical portion and top loading often make the system less dependent on the coax shield becoming the counterpoise.

In other words: the inverted-L structure itself supplies some of the “capacitive return behavior” that a flat-top/sloper EFHW often lacks unless you add it deliberately.

Why a Choke Alone Is Not Enough

Many operators try to solve EFHW instability by adding a common-mode choke. While a choke is essential to prevent coax shield radiation, it is not sufficient on its own—especially on lower frequencies like 160 m and 80 m.

A choke can impede common-mode current, but it cannot define a return path. If the antenna system still needs a place for imbalance current to go, it will find one... often by driving higher voltages, lighting up nearby conductive objects, or shifting where common-mode resonances occur.

This is generally less dramatic on higher bands (e.g., 20 m–10 m) because:

  • The antenna is electrically longer relative to many nearby objects, so small stray capacitances tend to have proportionally less effect
  • Coax lengths become a different fraction of a wavelength, changing (and often reducing) the severity of common-mode resonance cases
  • The transformer often sees a “friendlier” impedance range (lower effective Q in many real installs), so small environmental changes don’t swing the match as violently

Our Recommended Solution: Current Sink + Choke

For stable performance on flat-tops and slopers—especially from 160 m to 80 m—we recommend combining two things: a deliberate return path and a well-positioned choke.

Use a counterpoise wire (deliberate return path)

  • Any length is better than none
  • Run it away from the transformer/feedpoint area in as straight a line as practical (keep it predictable)
  • If you want an “earth bleed” point, you can terminate it into a corrosion-resistant RVS316 stainless steel ground rod

Add a 1:1 current choke at ~0.05 λ from the feedpoint

  • Based on the practical low-band findings popularized by DC4KU (Werner Schnorrenberg)
  • This placement aims to reduce common-mode current on the coax shield in a way that is repeatable

(Practical note: “0.05 λ” is band-dependent. As a rule of thumb, that’s ~8 m on 160 m and ~4 m on 80 m. For multiband operation you pick the lowest band you care about most, or choose a compromise.)

Reference: https://shop.rf.guru/pages/coax-length-before-the-choke-why-it-matters-for-efhw-antennas

Why the RVS316 Rod?

The goal here is not to create a “perfect RF ground” (that’s a different engineering problem). The goal is to provide a controlled leakage / bleed point so the system is less tempted to use your coax and shack as the counterpoise.

An RVS316 stainless steel rod is attractive in real installs because it offers:

  • Corrosion resistance and low maintenance (it stays mechanically and electrically consistent over time)
  • Higher resistivity than copper (so it tends to behave more like a lossy bleed point than a “low-impedance RF ground”)
  • Enough leakage to help drain imbalance and static without encouraging large differential currents to flow through your feed system

(The counterpoise wire is the main actor. The rod is a practical, durable “leak” into earth—not a miracle cure.)

Summary

Flat-top and sloper EFHW antennas are high-impedance, end-fed systems. That makes them:

  • Environmentally sensitive
  • More likely to drift under changing weather
  • Prone to common-mode issues if the return path is left undefined

A choke alone is not enough. For low-band EFHW antennas, combine:

  • A deliberate return path (counterpoise, optionally with a controlled earth bleed)
  • A well-placed choke (around ~0.05 λ on your lowest band of concern)

This combination improves stability, repeatability, and noise performance on 160 m and 80 m... and helps a flat-top/sloper EFHW behave like an antenna system instead of a “random RF experiment.”

Mini-FAQ

  • Is an EFHW always 2.5–5 kΩ? — No. It’s a common range for many end-fed half-wave installs, but height, end effects, nearby capacitance, and band/harmonic all shift the real feedpoint impedance.
  • Where should I connect the counterpoise? — At the transformer’s ground/counterpoise terminal (antenna side), not on the shack side of the choke.
  • How long should the counterpoise be? — There’s no universal number. Start with “something practical” (even 5–10 m helps on the low bands) and observe what improves stability and common-mode behavior in your install.
  • What does 0.05 λ mean in meters? — Roughly ~8 m on 160 m and ~4 m on 80 m. Pick the lowest band you care about most, or choose a compromise length.

Interested in more technical content? Subscribe to our updates for deep-dive RF articles and lab notes.

Questions or experiences to share? Feel free to contact RF.Guru for antenna and RF support.

Written by Joeri Van Dooren, ON6URE – RF engineer, antenna designer, and founder of RF.Guru, specializing in high-performance HF/VHF antennas and RF components.

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