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Electronics & Antennas for Ham Radio

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Antenna Impedance vs. Transmission Line Impedance

Related reading:
The Illusion of Resonance: When Coax Becomes the Antenna
Hybrid Baluns vs. Chokes in End-Fed and Off-Center Antennas
The Open-Wire Balanced Feedline: The Forgotten Ultra-Low-Loss Champion

Two numbers often confused in ham radio are the impedance of the antenna and the impedance of the feedline (coax or ladder line). While both use the unit of ohms, they describe fundamentally different physical realities. One is about how an antenna couples to free space, the other is about how a guided wave propagates in a medium. Conflating them leads to myths like “your antenna should be 50 Ω because coax is 50 Ω” — which is flat-out wrong.

What Antenna Impedance Really Means

An antenna’s input impedance is the ratio of RF voltage to current at its feedpoint when it is radiating. It is the result of:

  • Radiation resistance — the part that actually launches power into free space.
  • Loss resistance — real heat loss in conductors and dielectrics.
  • Reactive part — due to electrical length, capacitance, or inductance.

This impedance changes with frequency, environment, and geometry. A half-wave dipole in free space has ~73 Ω resistive impedance. An end-fed half-wave has several thousand ohms. Neither has anything inherently to do with “50 Ω.”

What Transmission Line Impedance Really Means

A transmission line’s characteristic impedance (Z0) is not a load; it is a property of the line itself. It is defined as the ratio of voltage to current of a traveling wave down the line when there are no reflections. For coax or ladder line, it depends on:

  • The geometry (diameter of conductors, spacing).
  • The dielectric constant of the insulating material.

RG-58 coax has Z0 ≈ 50 Ω, while common ladder line is 300–600 Ω. This number does not “match” the antenna — it simply describes the wave propagation environment inside the line.

Technical Note: Characteristic impedance is derived from Z0 = √(L′/C′), where L′ is inductance per unit length and C′ is capacitance per unit length of the line. Antenna impedance, in contrast, is derived from Maxwell’s equations and the boundary conditions of a radiating structure in space. Completely different physics.

How They Interact

Where the two meet — at the antenna feedpoint — is where mismatch occurs. If the antenna impedance ≠ line impedance, reflections happen. That’s what we see as SWR. The goal of matching networks, tuners, and baluns is to transform the antenna’s input impedance into something close to the line’s Z0 so power transfer is efficient and reflections minimal.

(Indicative: SWR itself is not “loss” — it’s the combination of mismatch and line attenuation that wastes power.)

Why Confusion Persists

Books, articles, and even some handbooks often phrase it poorly, suggesting that antennas are “designed for 50 Ω.” In reality:

  • Antennas are designed for efficient radiation — their impedance is a result, not a target.
  • Transmission lines are manufactured with convenient Z0 values (50 Ω, 75 Ω, 300 Ω).
  • The two only need a match at the junction to avoid reflections, not to share the same intrinsic value.

Key Takeaway

An antenna impedance is about interaction with free space. Transmission line impedance is about guiding waves inside a medium. Both are measured in ohms — but that’s where the similarity ends.

Mini-FAQ

  • Does coax “want” a 50 Ω antenna? — No. Coax has 50 Ω characteristic impedance regardless of what antenna you connect.
  • Why 50 Ω and not 75 Ω? — 50 Ω is a compromise between power handling and attenuation, chosen by convention in RF systems.
  • What happens if my antenna is 200 Ω? — With a 50 Ω coax, you’ll have a mismatch (SWR ≈ 4:1). Use a matching network or transformer to adapt.

Questions or experiences to share? Feel free to contact RF.Guru.

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

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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