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Electronics & Antennas for Ham Radio

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50 Ω Coax — Balanced at Its Design Impedance, Unbalanced When It’s Not

Coaxial cable is often called “unbalanced.” But the truth is more nuanced: it’s only unbalanced when it’s not operated at its design impedance.

Related reading:
Why antenna reciprocity is a mathematical theorem The ham’s obsession with resonance Do tuners tune the antenna? Resonance, conjugate match & Maxwell Understanding feedlines: coaxial & ladder line

Why coax is “balanced” at 50 Ω

Inside a coaxial cable, the fields are contained between the inner conductor and the inside of the shield. When the source impedance and the load impedance are both equal to the coax’s characteristic impedance (≈50 Ω for most ham gear), the currents on the inner conductor and the shield’s inner surface are perfectly equal and opposite. The cable is then balanced in the transmission-line sense, with no net external field leakage.

When coax becomes “unbalanced”

If either end of the cable is not 50 Ω, reflections appear. The shield current no longer exactly cancels the center conductor’s return current, and some energy flows on the shield’s outer surface as common-mode current. That’s what we call “unbalanced behavior.”

Key point: The word “unbalanced” in ham speak often refers to shield current leakage. In transmission-line theory, coax is fully balanced at its design impedance. It’s only when the terminations are mismatched that common-mode currents arise.

Coax as an impedance transformer

Any feedline is an impedance transformer. The impedance you measure at one end depends on the length of the line and what’s connected at the far end. That’s why coax length can appear to “shift resonance” of an antenna: it’s not changing the antenna, it’s transforming the impedance the shack sees.

This is why you may measure a dip in SWR at a different frequency at the rig than what exists at the feedpoint. The feedline transforms both the resistive and reactive parts of the load impedance.

Multiple SWRs inside a cable

A mismatched coax doesn’t have “one SWR.” Every point along the line has its own instantaneous impedance, cycling with line length. That’s why you can see different values depending on where you insert a meter. The reflection coefficient is the same, but the local impedance changes with position.

Using coax length as a matching tool

Because coax transforms impedance, deliberate use of line length can act as a simple matching element. A quarter-wave line, for instance, can invert impedances, while other lengths provide intermediate transformations. This is not “tuning the antenna,” but rather exploiting the feedline’s transformer behavior.

The need for chokes

If the system isn’t a perfect 50 Ω ↔ 50 Ω match, the coax outer surface becomes part of the antenna system. To suppress that, you need at least two common-mode chokes:

  • One at the feedpoint (to keep RF off the outer braid as it leaves the antenna).
  • One at the shack entrance (to keep any remaining common-mode off your gear).

Mini-FAQ

  • Is coax unbalanced? — At 50 Ω with matched ends, coax is balanced in its fields. Mismatch makes it behave unbalanced.
  • Why does coax shift resonance? — Because it’s an impedance transformer. The antenna’s feedpoint resonance appears shifted at the rig.
  • Can coax length be used for matching? — Yes, line length can transform impedances and help achieve a match at the rig.
  • Why two chokes? — One at the antenna and one at the shack entrance ensure common-mode currents are suppressed at both ends.

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.

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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