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Half-Wavelength Coax Myth — Why Quarter-Wave Tricks Actually Work

Updated October 2025

Related reading:
Why Minimum Coax Length Matters for Monoband Antennas
50 Ω Coax — Balanced at Its Design Impedance, Unbalanced When It’s Not

“Cut your coax to half-wavelength multiples.” Sound familiar? It’s one of ham radio’s oldest myths — and one that refuses to die. In truth, cutting your HF coax to ½ λ sections doesn’t fix SWR or “make things resonate.” It only repeats whatever mismatch your antenna already has. The real story is far more interesting — and where quarter-wave tricks actually do help, inside and outside the coax.

Why the Half-Wave “Rule” Is Wrong

Two facts from transmission-line theory led to decades of confusion:

  • Impedance repeating: a ½ λ section repeats the load impedance at its input (Zin=ZL). That’s true mathematically, but it doesn’t improve the match — it just mirrors it.
  • SWR invariance: SWR stays the same anywhere on a lossless line; only the phase of the reflection changes. On real, lossy coax, extra length may seem to lower SWR simply because it attenuates the reflection — hiding a bad match.

The “always use 18 ft” folklore may have worked on CBs, but it’s technically meaningless for SWR correction.

What a Quarter-Wave Section Really Does

Inside the coax, differential-mode signals follow:

Zin = Z₀ · (ZL + j Z₀ tan βl)/(Z₀ + j ZL tan βl).

At l = ¼ λ, this becomes an impedance inverter: Zin = Z₀²/ZL. That’s useful if you deliberately design a transformer with the right impedance, but not if you simply cut your 50 Ω coax to ¼ λ and hope for a miracle. The SWR magnitude remains unchanged; only voltage and current peaks move along the line — something tuners and ferrites care about.

Short coax jumpers often deliver the antenna’s raw impedance extremes straight into the tuner or transformer, exposing them to very high voltages or currents. Allowing the line roughly a quarter-wavelength of electrical length gives the impedance time to rotate into a more moderate region on the Smith chart. This rotation doesn’t change SWR magnitude, but it redistributes voltage and current nodes in a way that lets tuners and ferrite cores operate in a more comfortable zone — staying cooler and more linear under load.

The Forgotten Circuit: Common-Mode on the Outside

Unless properly choked, the outside of a coax shield becomes a third conductor that radiates. That’s why end-feds, OCFs, and verticals so often need multiple chokes. A physical ¼ λ of feedline (no VF correction, since the outer wave travels in air) can conveniently land a common-mode current node at the base if paired with a strong choke.

  • Install a 1:1 current balun near the feedpoint (≥ 3–5 kΩ CM impedance). This works best when the system includes a defined counterpoise of about 0.05 λ. If the coax shield itself forms the counterpoise, move the choke down the feedline by roughly the same 0.05 λ to align the current node correctly.
  • For stubborn RFI, add a second choke roughly ¼ λ (in air) down the feedline from the first choke to further suppress common-mode current.
  • Add a third choke before the coax enters the shack. This final barrier helps prevent residual common-mode current from coupling into indoor wiring or radiating out of the station on other equipment grounds.

Why Very Short HF Coax Runs Stress Tuners and Baluns

  • No rotation: extremely short coax doesn’t rotate the impedance much, exposing tuners and ferrites to the antenna’s raw extremes.
  • SWR illusion: longer coax can make SWR readings appear lower because reflections are attenuated. This doesn’t correct the mismatch at the antenna, but it can be a practical way to bring SWR within the range of built-in tuners that handle up to 3:1.

Practical Field Recipes

A) End-fed, OCF, or vertical setups

  • High-quality 1:1 choke near the feedpoint (≥ 3–5 kΩ CM impedance).
  • Optional second choke ~¼ λ down the feedline (in air).
  • Use at least ~¼ λ of coax (electrical) on your lowest band to ease tuner stress.

B) Center-fed balanced dipoles

  • With a proper feedpoint choke, coax length becomes a logistics and loss choice. No half-wave “magic.”

Static Quarter-Wave Reference Table

(Approximate physical ¼ λ lengths — adjust for actual coax velocity factor and installation.)

Band (MHz) ¼ λ inside coax (VF = 0.66) ¼ λ inside coax (VF = 0.85) ¼ λ outside (air)
1.85 26.76 m 34.46 m 40.54 m
3.60 13.75 m 17.71 m 20.83 m
5.30 9.34 m 12.03 m 14.15 m
7.15 6.92 m 8.92 m 10.49 m
10.13 4.89 m 6.30 m 7.41 m
14.20 3.49 m 4.49 m 5.28 m
18.10 2.73 m 3.52 m 4.14 m
21.20 2.33 m 3.01 m 3.54 m
24.94 1.98 m 2.56 m 3.01 m
28.50 1.74 m 2.24 m 2.63 m

Quick Choke Placement Cheat Sheet

  • Feedpoint choke: always mandatory. Aim for ≥ 3–5 kΩ CM impedance.
  • Second choke: place ~¼ λ (in air) down the coax from the first choke. Fine-tune by re-measuring CM current.
  • Third choke: before the line enters the shack to block residual currents in both directions.

Takeaway

The half-wave coax myth persists because it’s simple to repeat — but it’s wrong. A ¼ λ section, on the other hand, is genuinely useful when used intentionally: either as an impedance inverter inside the coax or as a current-node placer outside it. The key is understanding which circuit you’re acting on — differential or common-mode — and designing accordingly.

Mini-FAQ

  • Does coax length change SWR? — Not on a lossless line. It only rotates phase; SWR magnitude stays constant.
  • Why does longer coax “improve” SWR? — Losses attenuate reflections, faking a better reading at the rig.
  • Should I always cut coax to ¼ λ? — No. Use ¼ λ only when you need impedance rotation or choke placement.

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

Questions or experiences to share? Contact RF.Guru — we’d love to hear from you.

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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