EFHW AntennaDeep Research Report

PA3HHO Stacked Core Measurements Β· AI6XG VNA Methodology Β· RF.Guru Back-to-Back Myth Debunked Β· Trapped EFHW Design

BG1SB Knowledge Base | Synthesizing 25+ Authoritative Sources | 5 New Chapters Added

NEW 2643251002 Core Showdown Β· PA3HHO 4-Config Measurements Β· AI6XG 3-Step Separation Β· Trapped EFHW 20/30/40m

3:21 > 2:14 Winding 2643251002 Core PA3HHO Measured Data Trapped EFHW AI6XG VNA Methodology

01 / Fundamentals

EFHW Fundamentals & Impedance Characteristics

The EFHW (End-Fed Half-Wave) antenna is essentially a half-wave dipole fed at one end. Compared to center-fed dipoles, its core advantages are simple deployment β€” only one support point needed, feed point near the radio, and harmonic-based multi-band coverage.

// Impedance Characteristics

Key Physics Fact

The EFHW and dipole radiation patterns are nearly identical β€” both share the same current distribution. The EFHW is not a "magic antenna"; the only difference is the feed method and the resulting impedance matching challenge.

EFHW vs Dipole Comparison

CharacteristicEFHW (End-Fed Half-Wave)Center-Fed Dipole
Feed Impedance~2500 Ω, Needs 49:1 transformer~50-75 Ω, Direct coax
Support NeededSingle support pointCenter support + symmetric ends
Coax LengthVery short (feed near radio)Usually longer
Multi-BandHarmonic-based, no tunerNeeds tuner or multiple antennas
Transformer Loss0.3-3dB (depends on config)None
RFI RiskCMC suppression neededNaturally balanced, lower

02 / Transformer Design +3:21

49:1 vs 64:1 Transformer Design & Selection

Antenna Actual Impedance ÷ 50 = Ideal Transformation Ratio.Actual impedance is ~2000-3000 Ω, and 49:1 provides a universal compromise. But identical turns ratios do not guarantee identical performance β€” PA3HHO's measurements reveal a critical, long-overlooked variable: more primary turns dramatically improve low-band efficiency.

Turns Ratio Showdown: 2:14 vs 3:21

Characteristic49:1 (Traditional 2:14)49:1 (New 3:21)64:1 (2:16)
80m Loss (PA3HHO)2.3 dB (41%)0.3 dB (8%)N/A
40m Loss (PA3HHO)1.9 dB (36%)0.3 dB (8%)N/A
Efficiency ComparisonBaseline5× better on low bandsSimilar to 2:14
Best ScenarioObsoleted by new dataBest for 80-20mLow-band only

PA3HHO Key Finding (2025)

The 3:21 winding is 5× more efficient on low bands than 2:14. The mechanism: more turns β†’ higher inductive reactance β†’ lower magnetizing current β†’ dramatically lower core loss. On 80m, 3:21 loss is only 0.3dB (8%), while 2:14 reaches 2.3dB (41%). The trade-off is tighter winding space, which requires stacked cores to accommodate the extra turns.

Ferrite Core Selection

Research by RF.Guru and F5NPV reveals: no single core can maintain high efficiency across the entire 80m-10m range.

Core Materialμ ValueBest BandsRecommended Use
Type 43 (FT240)8503.5-14 MHzMost universal EFHW
26432510028503.5-14 MHzNew-gen dual-aperture: 90-93% efficiency
Type 77 (FT240)2000<10 MHz80m / 40m only
Type 52 (FT240)25014-30 MHz20m / 10m high bands
Type 31 (FT240)15001-20 MHzCMC choke only

RF.Guru Warning

Type 43 efficiency on 10m drops as low as 55%; Type 52 on 80m reaches only ~50%. The so-called "wideband 80-10m EFHW transformer" is more marketing promise than reality.

PA3HHO Recommendations Practical Guide

03 / Winding Methods

Winding Methods & W8JI Measurement Corrections

Traditional Twisted-Pair

  • First 2 turns of primary & secondary twisted together
  • Remaining turns coupled via core flux
  • Has crossover winding

Fuchs Split-Winding

  • Secondary wound alone on core
  • Primary wound alone between secondary
  • Needs 0.05λ counterpoise

Simple Parallel Winding (Recommended)

  • Primary & secondary wound in parallel
  • W8JI measured: better on HF
  • Distributed capacitance adds CM impedance

W8JI VNA Measurement Comparison Myth Debunked

FrequencySplit WindingParallel WindingWinner
15.71 MHz-33 dB-47 dBParallel +14dB
37.1 MHz-46 dB-41 dBSplit +5dB
134.8 MHz-19 dB-4.6 dBSplit +14dB
157 MHz-3 dB-11 dBParallel +8dB

"Many 'improvements' we just blindly accept from reading articles... The split winding often just shifts peak performance points higher in frequency."

— W8JI (Tom Rauch)

Key Conclusion

04 / CMC In-Depth

Common-Mode Choke (CMC) In-Depth Analysis

100W+ High Power

Must Use

Without CMC, the coax shield becomes part of the antenna system β†’ RFI into every appliance in the house

QRP (<10W)

Strongly Recommended

Problems are milder but still present β€” develop good habits to avoid chasing mysterious RF issues

CMC Placement

[Radio] ─── [Coax] ─── [CMC] ─── [49:1 Transformer] ─── [Antenna Wire] ↑ ↑ β‰₯3m from feed point 0.05λ counterpoise

Critical Warning

Never install CMC directly at the feed point, as it chokes the counterpoise and affects SWR. The ARRL Handbook recommends at least 10 feet (~3m) from the feed point.

BandFerriteFormTurns
80-20mMix 31FT240-315-9 turns RG-8X
40-10mMix 43FT240-436-10 turns RG-8X

RF.Guru VNA Warning NEW

Measuring coax shield common-mode impedance with a VNA does not prove choke effectiveness β€” shield current must be measured in the actual antenna installation. Bench VNA data cannot reflect real CMC operating conditions.

05 / Counterpoise

Counterpoise β€” Balance Ground

Common Misconception (PA9X)

"A half-wave EFHW doesn't need a counterpoise" β€” WRONG. No dedicated counterpoise β†’ coax shield β†’ radio chassis β†’ power supply β†’ every appliance ground β†’ entire house radiates RF.

Length Formula

L = 0.05 × λmax

40m→2m | 80m→4m | 160m→8m. Non-resonant length, sufficient to provide an RF return path without becoming a significant radiator.

AI6XG Minimalist Solution NEW

6ft RG316 coax = 0.05λ (40m). The coax segment between the transformer and CMC itself acts as the counterpoise β€” no extra wire needed.

06 / Multi-Band Mechanism

Multi-Band Harmonic Operation Mechanism

BandMultipleMatchNotes
40m1× λ/2BestFundamental resonance
20m2× λ/2GoodEven harmonic
15m3× λ/2PoorOdd harmonic
10m4× λ/2FairParasitic capacitance
30m/60m/17m/12m-InoperableNon-harmonic

WARC bands are inoperable. Chapter 12 trapped EFHW design solves the 30m problem.

// Typical SWR by band for 40m EFHW

07 / Real Performance PA3HHO Data

49:1 Transformer Real Performance & Loss Measurements

PA3HHO's systematic measurements reveal that configuration differences can cause up to 40% loss variation. This is currently the community's most comprehensive EFHW transformer efficiency comparison.

PA3HHO: Four-Configuration Measurement Comparison

Configuration80m40m20mPower
1×43 2:142.3dB (41%)1.9dB (36%)1.6dB (31%)100W
2×43 2:140.8dB (17%)0.7dB (15%)0.6dB (13%)200W
2×43 3:210.3dB (8%)0.3dB (8%)0.3dB (8%)400W PEP
3×52 2:140.1dB (1%)0.2dB (5%)0.4dB (9%)1kW PEP

The 3×52 Trade-off

3×FT240-52 achieves only 1% loss on 80m, but VSWR is elevated, requiring compensation components. Type 52 has narrow bandwidth and poor high-band matching. This is not a "perfect all-band solution."

"Low SWR does not equal high efficiency. An antenna at SWR 1.5:1 may be turning 30-50% of power into heat. A 100pF compensation capacitor improves SWR readings, not radiation efficiency."

— RF.Guru (ON6URE)

// PA3HHO Four-Configuration Loss Comparison (dB)

08 / Core Showdown NEW

Fair-Rite 2643251002 vs FT240-43

The 2643251002 dual-aperture core is a recent community highlight. SP9TKW and SurvivalComms reviews show efficiency reaching 90-93% (properly wound), 8-11% higher than single-core FT240-43.

Parameter2643251002FT240-43
Efficiency90-93%82-84% (single core)
Power300W SSB100W SSB (single core)
Inner Diameter16.75mm (tight space)35.6mm (ample space)
Turns Ratio56:1 (7.5:1)49:1 (7:1)
160-20mExcellentFair
10m+Steep drop-offFair
Efficiency Gain+8-11%Baseline

Core Trade-off

Conclusion

The 2643251002 is an excellent core, but not a wholesale replacement for FT240-43. 2×FT240-43 3:21 efficiency essentially matches 2643251002. Choice depends on winding ability and target bands.

09 / Stacked Measurements NEW

PA3HHO Stacked Core Measurement Comparison

PA3HHO (Pleun) conducted systematic measurements of four transformer configurations. This is the community's most comprehensive EFHW transformer efficiency comparison dataset.

Finding 1: Stacking Reduces Loss

2 cores: loss cut in half. 1×43β†’2×43, 80m from 2.3dBβ†’0.8dB. Doubled cross-section β†’ halved flux density β†’ exponentially reduced loss.

Finding 2: 3:21 Efficiency Leap

5× more efficient on low bands vs 2:14. More turns = higher inductive reactance = lower magnetizing current. The most underappreciated optimization.

Finding 3: Type 52 Triple Stack

Only 1% loss on 80m. But elevated VSWR and narrow bandwidth. N4LQ design reaches 1kW PEP.

Finding 4: Band-Specific Philosophy

43 for 80/40m, 52 for 20/15/10m. Band-specific optimization > all-band coverage.

// PA3HHO Efficiency vs Frequency (4 Configurations)

10 / Measurement Myth NEW

Back-to-Back Measurement Myth β€” RF.Guru Critique

RF.Guru (ON6URE) published an article in November 2025 that fundamentally exposed the flaws of "back-to-back" testing.

Popular Method (WRONG)

[Radio 50Ω] β†’ [Transformer A] β†’ [Transformer B] β†’ [Dummy Load 50Ω] "100W in, 94W out = 3W loss per transformer" "0.13dB β‰ˆ nearly lossless!" ← This is a placebo

Why It's Wrong

Back-to-Back Ideal Conditions

  • • Perfect 50Ω at both ends
  • • Symmetric structure cancels CM
  • • Purely resistive, zero reactance

EFHW Real-World Conditions

  • • Load 2-5kΩ + reactance
  • • Reactive current circulates as heat
  • • SWR 3:1-5:1
  • • Coax shield = third conductor

"Back-to-back testing only proves the transformer survives in easy-mode. 500W without smoke ≠ 500W efficient radiation."

— ON6URE, RF.Guru (2025-11)

Correct Evaluation Method

11 / VNA Methodology NEW

Correct VNA Measurement Method β€” AI6XG 3-Step Separation

AI6XG (Dan) proposed a rigorous methodology to decompose transformer loss into three independent components. This is key to distinguishing "bad transformer" from "antenna mismatch".

// AI6XG 3-Step Separation Method

Step 1: Mismatch Loss MM

MM = -10Β·log(1 - |S₁₁|²)

Reflection loss from impedance mismatch. Energy is reflected back to the transmitter, not turned into heat.

Step 2: Load Loss LL

LL = |S₂₁|² / (1 - |S₁₁|²)

Loss in the load resistor itself. Must first measure load complex impedance via Series-Through!

Step 3: Transformer Loss TL

TL = S₂₁ - MM - LL

The real transformer loss. This reflects the actual performance of the core, winding, and turns ratio.

Common Mistake

Assuming load is an ideal resistor β†’ efficiency calculated >100% on high bands (absurd). Without measuring actual load complex impedance, MM and LL cannot be correctly separated, making transformer loss calculation meaningless.

AI6XG Key Findings

12 / Trapped EFHW NEW

Trapped EFHW Design β€” Multi-Band, No Tuner Needed

AI6XG, K6ARK, and W2AEW have each developed trapped EFHW designs, solving one of EFHW's biggest pain points: no 30m WARC band coverage.

AI6XG 20m/30m/40m Trapped Design

[Transformer]──[9.4m]──[20m Trap]──[1.18m]──[30m Trap]──[2.06m] 20m: only 9.4m | 30m: 9.4+1.18m | 40m: all

Miniature Trap Parameters

TrapCapacitorCoilCoreResonant Freq
20m15pF NP039TT50-213.9 MHz
30m33pF NP037TT50-210.0 MHz

Measured SWR

1.2

20m

1.6

30m

1.2

40m

Design Comparison

DesignBand Change30mEfficiencyBest For
TrappedAutoYesHigherSOTA/POTA
LinkedManualOptionalHighestNo rush to change bands
Pure HarmonicAutoNoneModerateSimplest

If you need 30m and don't want an ATU, the trapped EFHW is currently the most elegant solution. K6ARK open-source design, total cost <$15.

13 / Dual-Mode Matching NEW

A+C Dual-Mode Matching System β€” A New Direction for Low + High Bands

A traditional single 49:1 ferrite transformer fails at both 80m (insufficient inductance) and 10m (capacitive-dominant, efficiency collapses to 55%). The A+C approach decomposes the problem: ferrite wideband transformer for low bands, powdered-iron resonant coupler for high bands, each playing to its strengths.

// System Architecture

ParameterUnit A (Low Bands)Unit C (High Bands)
Core2×FT240-43 StackedT200-2 Powdered Iron (Type 2)
MaterialMn-Zn Mix 43, μ=850Carbonyl Iron Powder, μ=10
Topology49:1 Wideband Transformer (3T:21T)AA5TB Parallel LC Coupler (3T:19T)
Band Coverage80m, 40m30m, 20m, 17m, 15m, 12m, 10m
BandwidthWideband, no tuningNarrowband (per-band variable capacitor tuning)
Efficiency Target~92% (0.3dB)90-95% (0.2-0.5dB)
Antenna Wire20m (same wire, DPDT switched)
Counterpoise4m (shared)

Why Ferrite and Powdered Iron Must Be Separate

The physical properties of ferrite Type 43 and powdered iron Type 2 determine their respective optimal frequency ranges:

PropertyFerrite (Type 43)Powdered Iron (Type 2)Advantage
μ (Permeability)85010Low μ = low core loss
Resistivity1-10 Ω·m10&sup5;-10&sup6; Ω·m (Granular insulation)T200-2: extremely low HF eddy currents
30MHz LossSignificantVery LowT200-2 wins
Temp StabilityFairExcellent (95ppm/°C)T200-2 wins
Saturation Flux~0.3T~0.8-1.0TT200-2: extremely hard to saturate
100W HeatingNoticeableAlmost no heatingT200-2 wins
BandwidthWidebandNarrowband (needs tuning)FT240-43 wins

Key Engineering Challenges

Quantitative analysis shows the A+C approach is theoretically sound (band-specific core materials), but the current prototype has 8 engineering challenges to resolve:

#IssueSeverityProposed Fix
1Non-resonant band impedance mismatch β€” 20m wire at 20m/10m is integer wavelength multiples, end impedance ~50-300Ω not ~2500ΩπŸ”΄ FundamentalAdd switchable turns ratio to Unit C
2Variable capacitor voltage rating inadequate β€” LC resonant boost effect yields V_peak of 1900-6300VπŸ”΄ SafetyVacuum variable capacitor (3-15kV)
3Counterpoise incompatibility β€” 4m at 10m = 0.38λ, becomes a radiatorπŸ”΄ SevereSwitch to 0.5m counterpoise for Unit C
4Variable capacitor outdoor reliability β€” condensation/corrosion/contact oxidation, 6-24 month lifespan🟑 ReliabilityVacuum cap + desiccant
5DPDT high-voltage switching β€” 707V peak exceeds 250VAC rating by 2×🟑 ModerateMove switching to 50Ω side
6Over-design β€” DMEGC Ni-Zn single core achieves 90%+ results at 1/5 cost🟑 DesignEvaluate single-core approach first
7Inter-unit parasitic coupling β€” idle unit absorbs ~2W🟒 MinorShort idle unit primary
8T200-2 core saturation🟒 Non-Issue39 gauss vs 800 gauss

Comparison with Simpler Solutions

Design80m40m20m10mComplexityCostReliability
Single FT240-43 2T:14TPoorGoodGoodFairVery Low¥50β˜…β˜…β˜…β˜…β˜…
DMEGC Ni-Zn μ=1000GoodGoodGoodGoodLow¥80β˜…β˜…β˜…β˜…β˜…
A+C Dual-ModeGoodGoodExcellent*Excellent*Very High¥400-600β˜…β˜…

* High-band efficiency advantage is ~0.2-0.4 dB, imperceptible in FT8 weak-signal modes. The real FT8 bottleneck is RX noise floor.

One-line summary: The A+C approach represents an important exploration direction β€” acknowledging the physical limits of single ferrite transformers and using band-specific multi-core designs to break through bottlenecks. The current prototype needs engineering iteration (HV switching, capacitor reliability, impedance matching range), but the direction is sound and worth continued exploration.

// Full analysis in EFHW knowledge base: efhw-knowledge/references/efhw_ac_dual_mode.md

14 / L-Network

L-Network Alternative Matching Solutions

VA3KOT compared 49:1 vs L-Network. A 49:1 autotransformer with 100pF capacitor is topologically an L-Network.

Comparison49:1 TransformerL-Network
BandwidthWideband multi-bandSingle-band
EfficiencyHas core lossHigher (no core)
PortableReady to useNeeds on-site tuning

15 / Radiation Patterns

Radiation Patterns & NEC Modeling

N6CC conducted in-depth NEC modeling analysis. The EFHW is the "last resort" for 80/60/40/30m regional coverage.

"High gain, wide bandwidth, small size β€” pick two. The EFHW in practice delivers none of the three."

— N6CC (Tim)

16 / Portable Β· Safety Β· Conclusions

PortableDeployment, SafetySafety &Key Conclusion

2026 Portable Products Updated

ProductBandsPowerFeatures
Spooltenna Ultra40/20/15/10m100W SSB162g open-source
AI6XG Trapped40/30/20m5W QRPNo-tuner SOTA
K6ARK Mini40/20/15/10mQRPTransformer built into BNC connector
Chameleon LEFS40/20/15/10m25W SSB113g

High-Voltage Safety

Quick Deployment Tips

Key Conclusion (Supplement Edition)

01 3:21 > 2:14

Same 49:1 turns ratio, 3-turn primary is 5Γ— more efficient on low bands. The most underappreciated optimization.

02 Band-Specific Design

Avoid pursuing full 80-10m coverage. Use 43 for 80/40m, 52 for 20/15/10m.

03 Optimal Balanced Solution

2Γ—FT240-43 3:21, only 0.3dB loss across all bands, 400W PEP.

04 Measurement & Bottom Line

Back-to-back testing is a placebo. CMC + 0.05λ counterpoise are non-negotiable. Low SWR β‰  high efficiency.

05 Trapped Design

Trapped EFHW solves the 30m problem. AI6XG/K6ARK designs are open-source, cost <$15.

06 VNA 3-Step Method

AI6XG: measure load complex impedance first, then separate MM/LL/TL. Assuming ideal resistor β†’ efficiency >100% error.

17 / System Architecture NEW

EFHW Fuchs ATU V3.0 β€” Premium Architecture Board

The premium board splits the system into two real chains: the RF/DC physical path and the measurement/control loop. The ATR1000 sits explicitly behind the radio and before the Bias-T, at the shack-side reference plane; the remote ATU is only an actuator, and tuning quality is observed indirectly through the near-end SWR meter.

01 Β· RF/DC physical path Series order is the architecture: Radio β†’ ATR1000 β†’ Bias‑T β†’ coax β†’ remote ATU β†’ EFHW Radio TX source 100W PEP Β· 5W tune 50Ξ© output ATR1000 SWR / power coupler SHACK-SIDE REFERENCE PLANE physically near / stacked with radio series element before Bias‑T Indoor Bias‑T DC injection box C block + RF choke 13.8V rides on coax Long coax feedline RF + DC transport loss / delay matters Outdoor EFHW ATU remote servo Fuchs coupler ACTUATOR, NOT A METER ESP32-S3 drives MG996R moves 10–500pF air capacitor near antenna feed point EFHW antenna wire ~20m + counterpoise measurement data leaves RF path here 02 Β· Measurement/control loop The loop is remote-action / local-observation: servo changes antenna-system impedance, ATR1000 observes the result at the radio end. ATR1000 SWR + forward power radio-side sample MRRC reads meter orchestrates scan WebSocket WiFi JSON control tune_start / swr_update remote command path to ESP32 03 Β· Remote ATU internals Low-voltage controller and high-voltage RF tank are separate physical domains. OUTDOOR UNIT BOUNDARY Bias‑T extract12V / 6V / 3V3Bias‑V ADC ESP32‑S3FreeRTOS tasksNVS + LEDC PWM MG996Rservopower cut Fuchs LCT200‑6 2:14Tair cap β‰₯5kVoff‑PCB HV wiringarc not locally sensed 04 Β· Engineering semantics Measurement plane best_swr is ATR1000 / shack-plane SWR. Not capacitor voltage. Not ATU output SWR. It optimizes what the radio sees through the feedline. Control loop Each servo step waits for a new swr_update. Network jitter, MRRC polling, meter latency directly shape sweep duration and curve quality. Tuning algorithm NVS hit β†’ direct position; miss β†’ sweep. 37 coarse samples @5Β° + 30 fine steps @1Β° then save freq β†’ servo_pos Β±50kHz fuzzy. Safety boundary Abort on overpower / no RF / high SWR / timeout. Still not directly detectable: RF arc, tank heat, servo position/current, water ingress, HV stress. servo move β†’ RF impedance changes β†’ shack-side SWR changes β†’ next update

Topology accuracy

The ATR1000 is drawn as a near-end coupler on the RF main path β€” behind the radio, before the Bias-T β€” and is no longer mistakenly placed as a side sensor on the outdoor ATU.

Clear reference plane

Every SWR optimization is based on the radio-side reference plane. The remote ATU's effect reflects back through the long coax to this plane, where MRRC reads it.

Auditable control path

The RF physical path and the WebSocket control path are drawn as separate layers, exposing every latency / failure point: meter read, MRRC, WiFi, ESP32, servo.

No safety overclaim

The diagram deliberately keeps the "not directly detectable" boundary: capacitor arcing, tank heating, real servo position, current and water ingress cannot be substituted by ATR1000 sensing.