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.
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.
| 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.
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.
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