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Faraday Strip Radials: 23% of What, Measured Where?

A relative number needs a baseline

Faraday Strip Radials: 23% of What, Measured Where?

A portable radial strip may be convenient, visible and repeatable to deploy. It may also change the measured field. But “23–28% more relative field strength” is not yet an efficiency result: first we need to know which quantity changed, which wire system formed the baseline and how the complete antenna was measured.

ON6UREVertical antennasRadialsField strengthDecibelsN6LF
Related reading from RF.Guru
Radials Have Two Jobs: Return Current and Field Control Short Radials and Rudy Severns: Read the Test Before the Rule Can Two Radials Really Add 4 dB?

RF.Guru working definition: Common-mode current is the non-cancelling phasor-sum current in a specified set of conductors, evaluated at a defined cross-section and using a declared current-direction convention. In the intended differential transmission-line mode, the outgoing and return currents are equal and opposite, so their phasor sum is zero. When they do not cancel, the remaining current must close through another reference or return path—such as the outside of a coax shield, a mast, equipment chassis, station wiring, nearby structures, earth, the operator, or distributed coupling through the environment.

This broader working definition is especially useful in practical antenna systems. On transmit, non-cancelling current on the outside of the coax can make the feedline and connected structures part of the radiating antenna system unless that path is intentional, clearly defined and properly controlled—for example by providing the required return path and placing a suitable common-mode choke at the correct boundary.

Chameleon Antenna describes its CHA FSR as two 20-foot conductive strips laid in an X. Its public product page reports a median 23–28% increase in relative field strength in initial Northern Alabama tests, compared with the four 12.5-foot wire radials supplied with two named vertical systems. That is the claim I am examining. I am not arguing that a strip cannot work. I am asking what the published number proves.

My practical objection: a percentage without the starting system can make a modest conditional difference sound universal. Twenty-three percent more than an undefined or weak baseline does not tell us the absolute radiation efficiency, the pattern, or whether another wire layout using the same weight, footprint or deployment time would do better.

Start With the Quantity

Electric-field strength is an amplitude, normally expressed in volts per metre. Power and power density are different quantities. The two decibel conversions are:

Amplitude ratio: ΔdB = 20 log10(E2/E1)

Power ratio: ΔdB = 10 log10(P2/P1)

Meaning of the reported percentage 23% increase 28% increase
Electric-field amplitude ratio 20 log10(1.23) = 1.80 dB 20 log10(1.28) = 2.14 dB
Power ratio 10 log10(1.23) = 0.90 dB 10 log10(1.28) = 1.07 dB

If 1.23 or 1.28 is the electric-field ratio in a far-field plane wave, power density scales with E². The corresponding power-density ratios are about 1.51 and 1.64, which still produce the same 1.80 dB and 2.14 dB results. We must not apply 10 log to an amplitude percentage or 20 log to a power percentage.

Nor should we translate either result casually into “one-third of an S-unit.” S-meter response is receiver-, band-, mode- and calibration-dependent; fading and noise add further variability. A repeatable 2 dB field change is not nothing, but an S-meter slogan does not tell us whether it matters to a particular link.

The Claim Is a Comparison, Not an Efficiency Rating

The manufacturer identifies a useful comparison: its two-strip system versus four 12.5-foot wire radials. The public page does not publish enough of the initial field-test protocol to turn that comparison into a general antenna-efficiency number. At minimum, a reproducible result needs the band, radiator and matching configuration, accepted feedpoint power, feedline and choke boundary, radial orientation, soil and moisture, probe distance, bearing, height, polarisation, sequence, repetitions, raw observations and uncertainty.

A field-strength difference at one position can come from a change in total radiated power, elevation or azimuth pattern, common-mode current, matching loss, radiator current, or coupling to the measurement setup. It cannot by itself separate those causes. An input SWR change cannot separate them either.

The claim may be perfectly repeatable for the named Chameleon systems and test sites. It still does not establish that strip radials universally add 23–28%, or that the completed antenna has a particular absolute efficiency.

A Wide Strip Changes More Than Resistance

Width can matter. In Rudy Severns' primary study of copper-foil conductors, a finite-element model at 14 MHz showed conductor loss falling as 0.008-inch copper foil was widened from 0.125 inch to 1 inch. The improvement did not scale as simply as DC cross-sectional area because RF current was not distributed uniformly across the strip.

That result supports a bounded statement: conductor width can reduce AC loss in a declared material, thickness, frequency and current geometry. It does not prove that every conductive fabric has lower loss than every wire, or that lower strip resistance becomes an equal reduction in soil loss for the completed antenna.

A ground-contact strip can also change distributed capacitance, soil current density, radial resonance, feedpoint impedance and current division. Its fabric, plating, seams, grommets and contact resistance matter. Laying two strips in an X creates four physical arms, but that does not make them electrically equivalent to four independent wires—or to eight, sixteen or thirty-two wires. Measure the current instead of counting shapes.

What Rudy Severns Actually Measured

The N6LF experiments are often reduced to “more short radials are better.” Rudy's data say something much more useful and much less universal.

In Experimental Determination of Ground System Performance for HF Verticals, Part 2, one test used a 34-foot aluminium vertical at 7.2 MHz with four insulated surface radials varied from 33 feet to 18 feet. Feedpoint impedance, relative transmission and radial-current division were measured, and a common-mode choke isolated the antenna from the feedline and ground. Shortening those four radials towards roughly 23 feet improved the measured result in that installation because the sparse soil-loaded screen had a loss-producing resonance.

In the follow-on comparison, Rudy re-resonated an adjustable vertical as 4, 8, 16 and 32 radial fields were changed between 33-foot and 21-foot wires. The shortening advantage diminished as count increased. With 32 radials, the longer set was 0.12 dB ahead in that particular experiment. That is the opposite of a universal “shorter always wins” rule.

In Part 4, a fixed-wire comparison on a top-loaded one-eighth-wave vertical at 7.2 MHz found nearly the same relative signal from sixteen 33-foot radials and thirty-two 17-foot radials. The feedpoint impedances differed, and the radiator was lengthened to restore resonance for the shorter set. More shorter wires can therefore be an effective allocation of a fixed conductor budget in a particular installation. They are not automatically superior.

Elevated and Surface Radials Are Different Systems

Another N6LF result is routinely detached from its conditions. Part 3 of the 2009 series compared a 64-radial surface system with four carefully balanced radials elevated 48 inches in one controlled 7.2 MHz installation. Their normalised transmission results differed by only 0.1 dB.

That experiment does not establish a fixed 0.05–0.1λ height or prove that four elevated radials always equal a dense surface field. In his 2012 elevated-ground-system study, Rudy stressed the sensitivity of a four-radial fan to asymmetry, soil and nearby conductors. He recommended 10–12 or more elevated radials for robustness in that design context.

Surface radials couple strongly to the ground. Elevated radials are coupled antenna elements whose current balance, resonance and geometry can reshape the pattern. A count taken from one cannot be assigned to the other.

There Is No Fixed Loss Table by Radial Count

Four, eight, sixteen or thirty-two wires do not have an intrinsic loss in decibels. The result depends on radiator current, frequency, radial length and distribution, soil, matching network, conductor loss, feedline common mode and the measurement reference plane.

Radiation efficiency is a power ratio:

η = Pradiated / Paccepted

Efficiency in dB = 10 log10(η)

To calculate that ratio, we must know or estimate the radiated power and every relevant loss term. Feedpoint resistance is not automatically “ideal radiation resistance plus ground loss,” because the radiation resistance and current reference can change with the installed ground system. A low SWR says nothing by itself about η.

A Fair Strip-versus-Wire Test

  1. Define the comparison. Equal conductor mass, equal footprint, equal deployment time, equal cost and equal radial count are different engineering questions.
  2. Hold the radiator fixed. Record radiator length, height, loading, matching network, feedpoint and nearby conductors.
  3. Control accepted power. Measure at a declared reference plane and correct for feedline and matching loss.
  4. Control the return boundary. Characterise the choke and map current on the coax exterior before and after it.
  5. Record the radial system. Include material, resistance, strip or wire dimensions, orientation, contact condition, soil and moisture.
  6. Map current. Compare branch current and phase where practical; an input match can hide unequal or unintended return paths.
  7. Measure remote field consistently. Use the same calibrated probe, distance, height, bearing and polarisation; test more than one bearing if pattern change is possible.
  8. Use A/B/A restoration. Reinstall the baseline and confirm that time, weather, soil or placement did not manufacture the improvement.
  9. Publish uncertainty and raw ratios. A median without sample count, spread or measurement uncertainty is not enough to judge repeatability.

Portable Value Is Not Only a Decibel

A radial system can earn its place because it deploys quickly, stays organised, is visible around people, survives repeated use or recreates the same geometry at every site. Those are legitimate system requirements. Weight, packed volume, drying, repair and trip management are legitimate costs.

Keep those mechanical advantages separate from RF proof. “Convenient and repeatable” can be the deciding result without inflating a conditional field comparison into a universal efficiency claim.

Primary Evidence

  • Chameleon Antenna — CHA FSR product page: manufacturer wording, comparator, strip layout and reported 23–28% relative field-strength result.
  • NIST Special Publication 250-32: decibel relationships for power and equal-impedance voltage ratios.
  • ITU-R SM.329-8: field-strength and power-flux-density units and relationships.
  • ARRL — Test Procedures to Measure BPL Interference: field-strength measurement geometry, probes and S-meter limitations.
  • Rudy Severns, N6LF — Resistance of Foil Conductors for Antennas: frequency-, width-, material- and current-distribution boundaries for foil loss.
  • Rudy Severns, N6LF — Ground System Performance for HF Verticals, Part 2: sparse surface radial length, count, resonance and current measurements.
  • Rudy Severns, N6LF — Ground System Performance for HF Verticals, Part 4: radial-count and fixed-wire comparisons.
  • ITU-R P.527-6 — Electrical Characteristics of the Surface of the Earth: frequency-, material-, moisture- and temperature-dependent ground properties.

Practical Conclusion

A reported 1.8–2.1 dB field-amplitude difference would be measurable and potentially useful. It is not “nothing.” But the engineering question remains: relative to what, at which frequency, with which radiator, return path, accepted power, soil, probe position and uncertainty?

I will not pretend that a strip cannot outperform four short wires. I will also not turn that comparison into “strips are more efficient” or answer it with the opposite folklore that more short wire always wins. Width, length, count, material, geometry and soil all move the installed currents. Put the baseline and the measurement method beside the percentage; then the number can finally speak.

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

  • Does 23% more field strength mean 23% more power? No. If 23% is an electric-field amplitude increase, it is 1.80 dB and corresponds to about 51% more far-field power density. If 23% is already a power ratio, it is 0.90 dB.
  • Is a 1.8–2.1 dB field difference nothing? No. It is measurable and may matter near a link margin. Its practical value depends on repeatability, uncertainty, fading, noise and whether the pattern changed.
  • Does a wider radial always lower antenna-system loss? No. Width can reduce conductor loss in a specified material and geometry, but soil coupling, current distribution, connections, radial resonance and the rest of the antenna determine the system result.
  • Are more short wires always better than fewer long wires? No. N6LF measured cases where distributing fixed wire among more shorter radials worked well, but the result changed with count, radiator, soil, frequency and retuning.
  • Do four elevated radials always equal 64 surface radials? No. They differed by only 0.1 dB in one controlled N6LF 7.2 MHz experiment. Sparse elevated systems remain sensitive to balance, soil and nearby conductors.
  • How should strip and wire radial systems be compared? Hold radiator and accepted power constant, control feedline common mode, record soil and exact geometry, map current, measure remote field at repeatable positions and restore the baseline with an A/B/A sequence.

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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