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Carbon Fixed Size Whips for the 10M/20M band vs Stainless Slider Whip

An evidence-based comparison using real-world measurements: why carbon looks “wideband,” what that actually means for TX efficiency, and why RX barely notices.

Related Reading
Carbon Radiators — Miracle Antenna or Marketing Smoke?
Carbon Fiber Antenna Elements (Not Masts) vs Stainless Steel

Weight vs Loss — Carbon Fixed Length Whips vs 5.2 m – 10.35 m (17–34 ft) Stainless Slider

TL;DR: Carbon whips are extremely light but essentially fixed-band tools: an ~89 in (~2.26 m) rod lands near 10 m, and a ~201.6 in (~5.12 m) rod lands within 20 m (no series element required in our 20 m tests). A 34 ft (10.35 m) stainless telescopic whip is heavier, but covers 10–40 m by simply sliding to resonance — no tuner, no traps, no loading. It also becomes an inverted-L for 80/160 m with a small base L-match, transmatch or loading coil and a wire attached to the top. Smaller stainless slider whips like 17 ft (5.2 m, 20 m band) or 25 ft (7.62 m, 30 m band) can also be used as inverted-Ls, but they are less efficient than the 34 ft (10.35 m) version.

Core ideas

  • Carbon vs metal losses: Carbon radiators are lossier, but on 10/20 m near quarter-wave length the penalty is modest.
  • RVS slider = tuner-free agility: A 34 ft stainless whip covers 10–40 m with no traps, no loading, no transmatch — just slide to resonance.
  • Carbon = fixed lengths: Off 10/20 m, carbon rods need a base tuner.
  • 80/160 m: The 34 ft RVS converts easily into an inverted-L via a top wire and a small base L-network or transmatch.

Band coverage cheat-sheet

Band Carbon fixed whip RVS (34 ft slider) Notes
10 m ~89 in carbon + small series C Slide to resonance — no tuner Quarter-wave region; high efficiency with good radials.
12/15/17 m Requires transmatch Slide to resonance RVS allows multi-band agility without added hardware.
20 m ~201.6 in carbon (no series element needed) Slide to resonance SWR < 1.5 across 14.0–14.35 MHz in our tests.
30/40 m Requires transmatch Slide to resonance Full band coverage via length alone (for the 34 ft (10.35 m)).
40/80/160 m Needs transmatch Inverted-L + small base L-match or transmatch Very field-friendly configuration.

Weight planning by scenario

Scenario What you carry Typical weight*
Single-band carbon 10 m or 20 m + gram-level matching 45–70 g
Two-band carbon 89 in + 201.6 in + tiny series elements 100–150 g
Carbon + base tuner One whip + 150–350 g tuner 190–420 g
RVS 34 ft 10–40 m One stainless slider 500–900+ g
RVS inverted-L (80/160 m) Slider + top wire + small L-match or transmatch 550–1050+ g

*Radials, feedline, mounts excluded.

Matching specifics (quick)

  • Carbon 10 m: base series capacitor cancels +jX.
  • Carbon 20 m: no series element needed.
  • Carbon other bands: requires a base transmatch.
  • RVS 34 ft 10–40 m: Slide to resonance — no tuner needed.
  • RVS 80/160 m inverted-L: add top wire + small base L-match.

Scenario guidance

  • Single band: Carbon + fixed match → ultra-light.
  • Two bands: Two carbon whips, or RVS slider for no-tuner operation.
  • 80/160 m: RVS inverted-L is drastically easier and far more efficient than carbon.

Takeaway

If you care about grams, go carbon. If you want tuner-free 10–40 m agility (and simple 80/160 m capability), a 34 ft stainless slider is the most versatile field whip available.

Measured Performance of Carbon vs Stainless Resonators

Carbon resonator

Same physical length as RVS

  • 33.6 MHz, SWR 1.50, RL 14 dB
  • Z ≈ 45.6 + j19 Ω (|Z| ≈ 49.4 Ω)
  • L ≈ 90 nH
  • Series C to cancel +jX ≈ 249 pF

Stainless (RVS) resonator

  • 32.2 MHz, SWR 1.29, RL 18 dB
  • Z ≈ 45.6 + j11.2 Ω (|Z| ≈ 46.9 Ω)
  • L ≈ 55 nH
  • Series C to cancel +jX ≈ 440 pF

After cancelling the small inductive component, the remaining resistive term is ~45.6 Ω — an excellent match to 50 Ω. This does NOT mean both antennas are equally efficient. It only means the feedpoint impedance looks similar.

20 m Version — Real-World Measurements

With both elements at the same physical length (RVS slider set to match the carbon rod), we measured the following around the 20 m band.

Summary (center of band ~14.2 MHz)
Parameter @ 14.2 MHz Carbon Stainless (RVS)
SWR / Return loss 1.45 / 14.7 dB 1.47 / 14.5 dB
Impedance Z ≈ 38.7 − j12.1 Ω (|Z| ≈ 40.5 Ω) Z ≈ 41.9 − j15.6 Ω (|Z| ≈ 44.7 Ω)
Phase (Γ) ≈ 0.2° ≈ 0.2°
Series-equivalent C from X<0 ≈ 929 pF (from −j12.1 Ω) ≈ 716 pF (from −j15.6 Ω)
SWR dip (min) ≈ 14.3 MHz ≈ 14.1 MHz

Band coverage: Both antennas show SWR < 1.5 across the entire 20 m band (14.0–14.35 MHz). No series matching element is required.

What this tells us

  • Both behave like healthy near-¼-wave monopoles: resistive parts ~39–42 Ω with a small capacitive term (a hair “short” at 14.2 MHz).
  • If you want X→0 exactly at 14.2 MHz, a tiny series L would do it (carbon ≈ 0.136 µH, RVS ≈ 0.175 µH) — but it’s unnecessary given the already low SWR.
  • Carbon’s SWR bandwidth is slightly wider than RVS (lower Q due to higher loss), but on 20 m the effect is modest compared with 10 m.

Why the differences on 20 m are small

  • Geometry dominates. Near ¼-wave, radiation resistance is ~36–40 Ω; a few ohms of extra loss barely moves SWR or resonance.
  • Small resonance split. The ~200 kHz delta (~1.4%) between the dip frequencies reflects a tiny difference in effective electrical length — only ~7 cm on a ~5.1 m element.
  • Bandwidth hides small changes. With FBW ≈ 2.5% for 1.5:1 SWR across the band, the implied loaded Q ≲ 47; carbon vs RVS Q shifts of a few percent are hard to see.

Why Carbon Looks “Wideband” on a VNA

Carbon-fiber and graphite composites have significantly higher RF resistance than metal. Higher RF resistance → more loss → lower Q. Lower Q → the SWR dip becomes wider.

This is a measurement artifact: a wide SWR dip is the hallmark of loss, not “built-in broadband magic.”

Carbon also shifts the resonance higher (33.6 vs 32.2 MHz) because loss changes current distribution and effective electrical length.

RX vs TX — Why Receive Barely Cares

At 1–35 MHz, man-made + atmospheric noise dominates the receiver noise floor. Antenna efficiency differences of 1–3 dB rarely change SNR. On transmit, however, every dB you lose in the radiator is a dB not radiated.

Matching the Two Whips

Carbon (fixed length)

  • On 10 m → series C
  • On 20 m → none required
  • Other bands → a base transmatch

Stainless RVS (adjustable)

  • Tune by sliding → no tuner required on 10–40 m
  • For 40/80 → inverted-L with small base L-match

Efficiency Comparison

(Representative values for Ø 6 mm rods at 33.6 MHz; exact numbers depend on geometry and ground system.)

Near-quarter-wave whip (~2.2 m)

Radiation resistance ≈ 36.5 Ω. Ground loss ≈ 2 Ω.

Efficiency η = Rrad / (Rrad + Rcond + Rground + Rtuner)

Material / Tuner η (no tuner) η (light match) η (heavy transmatch) Loss vs RVS
RVS 92.1% 92.0% 90.5% —
Carbon (σ = 2×10⁵) 87.9% 87.8% 86.0% −0.20 dB
Carbon (σ = 1×10⁵) 85.4% 85.3% 84.0% −0.33 dB
Carbon (σ = 5×10⁴) 82.0% 81.9% 80.8% −0.50 dB
Carbon (σ = 2.5×10⁴) 77.7% 77.6% 76.7% −0.74 dB

A Nuance Worth Discussing — Weight vs Loss

Carbon is lossier — but it is extremely light. For SOTA/POTA/QRP field operations, a carbon whip plus a small fixed series capacitor for one band can be dramatically lighter than carrying a stainless whip + tuner.

  • No tuner needed on 10 m with a fixed series-C match; 20 m required no extra matching in our tests.
  • Fixed C weighs under 2 g.
  • Carbon whip weighs 40–65 g vs 180–230 g for stainless.

For fixed stations, stainless wins. For ultra-light portable work, carbon often wins.

Technical Note — Weight vs Efficiency Trade-off

A stainless whip (~2 m, Ø 6 mm) typically weighs 180–230 g. A carbon equivalent weighs 40–65 g. A fixed matching capacitor adds <2 g. A portable tuner adds 150–350 g + coax loss.

For SOTA/POTA/QRP, saving 250–450 g of pack weight is often worth more than losing 0.7–1.5 dB in TX efficiency.

Takeaway: For lightweight field ops on 10 m and 20 m, carbon + fixed matching is often the smarter choice.

Simple Lightweight Matching for 10 m (Carbon Whip)

The principle

Your carbon whip shows a small +jX on 10 m. A single series capacitor cancels that inductive reactance.

Carbon @ 33.6 MHz → X = +19 Ω → C ≈ 249 pF

Component recommendations

  • Use C0G/NP0 or silver-mica capacitors.
  • At least 100 V RF rating (more for QRO).
  • Place directly at the base feedpoint.

Advantages

  • No tuner → zero added loss.
  • Only grams of parts.
  • Stable match across the 10 m band.
  • Perfect for ultralight SOTA/POTA.

A full 10 m carbon system (whip + fixed C + clamp) can weigh under 70 g total.

Carbon vs Stainless — At-a-Glance Comparison

Property Carbon Composite Stainless Steel (RVS)
Conductivity 10–100× lower (lossier) Better, but lower than copper
Weight Extremely light Heavy
Q / Bandwidth Lower Q → wider dip Higher Q → narrower dip
Matching Needs Often needs matching Often none (slide)
Best For Portable, QRP, 10/20 m Fixed/mobile, multi-band
RX Performance Noise-limited → same Excellent
TX Efficiency 0.3–1.6 dB lower Higher
Durability Strong but brittle Very durable
System Weight Smallest possible Heavier, especially with hardware

Mini-FAQ

Quick Answers

  • Does carbon radiate worse? — Yes. Its conductivity is 10–100× lower than metal, so efficiency is always lower.
  • Is carbon okay for receive? — Yes. At 1–35 MHz external noise dominates SNR, so RX performance is basically identical.
  • Why is the SWR dip wider on carbon? — Because loss → lower Q → broader dip. It looks good on a VNA, but it’s a loss effect.
  • Can a carbon whip be matched with a single capacitor? — On 10 m, usually yes. A small NP0/C0G or silver-mica series capacitor cancels +jX.
  • When does stainless clearly win? — Multi-band work (10–40 m) and anything involving 40/80 m (as an inverted-L).
  • When does carbon win? — When weight is the priority (SOTA/POTA/QRP) and you operate mainly on 10 m or 20 m.

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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