Corrugated Cable
How Corrugated Coaxial Cable Achieves Hardline Performance
The defining feature of corrugated cable is its outer conductor: instead of the woven copper braid found in flexible RG-style coax, the shield is a continuous seamless copper or aluminum tube that has been mechanically corrugated. The corrugations are what make a thick-walled metal tube flexible enough to ship on a reel and pull through a cable tray, yet the tube remains a solid conductor with no braid gaps. That gives shielding effectiveness above 120 dB and eliminates the braid-leakage and triboelectric noise that plague flexible cables, while the large tube diameter lowers conductor loss because skin-effect resistance per unit length falls as the conductor circumference grows.
Inside the tube, the center conductor is a smooth or corrugated copper tube or solid copper wire, supported by either a closed-cell foam polyethylene dielectric or an air-spaced spiral spacer. Both dielectric systems target a relative permittivity near 1.2 to 1.5 and a loss tangent below 0.0003, which is why corrugated cable approaches the loss of air-filled rigid line. Because the dielectric is mostly air or gas-blown foam, the cable must usually be sold with a sealed jacket or kept pressurized with dry air or nitrogen to keep moisture out, since water ingress raises both attenuation and the dielectric loss tangent dramatically.
Two corrugation geometries dominate. Annular cable has independent rings stamped around the circumference and delivers the lowest attenuation and cleanest return loss, at the cost of a larger minimum bend radius. Helical cable uses a continuous spiral, behaving like a coarse screw thread, which yields a much tighter bend radius and faster installation but introduces a small periodic structure that designers keep resonance-free across the operating band.
Attenuation and Velocity Factor Relations
VF = 1 / √εr ≈ 0.84 to 0.92 (for εr ≈ 1.18 to 1.42)
Total Feedline Loss:
Ltotal = α × (length / 100) dB, with α in dB/100 m
Conductor-Loss Frequency Scaling:
αc ∝ √f (skin effect, below dielectric-loss onset)
Helical Corrugation Resonance (avoid in band):
fres ≈ c × VF / (2 × p) where p = corrugation pitch
Example: 7/8" cable is ≈ 1.1 dB/100 ft (3.6 dB/100 m) at 1 GHz, so at 2 GHz the √f scaling gives α ≈ 5.1 dB/100 m; a 60 m run then loses Ltotal ≈ 3.1 dB. Pitch p = 8 mm, VF = 0.88 → fres ≈ 16.5 GHz, far above any 2 GHz band.
Corrugated Cable Size and Performance Comparison
| Cable Size | Atten. @ 1 GHz | Avg Power @ 1 GHz | Min Bend Radius | Velocity Factor | Typical Use |
|---|---|---|---|---|---|
| 1/2 inch | ~2.3 dB/100 ft | ~0.8 kW | 32 mm (helical) | 0.88 | Jumpers, tower-top runs |
| 7/8 inch | ~1.1 dB/100 ft | ~2.5 kW | 120 mm (annular) | 0.89 | Base station main feeder |
| 1-1/4 inch | ~0.8 dB/100 ft | ~4 kW | 200 mm (annular) | 0.90 | Broadcast, long runs |
| 1-5/8 inch | ~0.6 dB/100 ft | ~6 kW | 250 mm (annular) | 0.92 | High-power FM/TV |
| RG-213 (braided, ref.) | ~6.5 dB/100 ft | ~0.3 kW | 25 mm | 0.66 | Short patch leads |
Frequently Asked Questions
What is the difference between annular and helical corrugated cable?
Annular cable has independent ring-shaped corrugations and gives the lowest attenuation and cleanest return loss, but it is stiffer with a larger bend radius (10 to 20 cable diameters). Helical cable uses a continuous spiral corrugation, so it flexes far more easily and bends to 5 to 8 diameters, at a small attenuation penalty. The helical pitch creates a periodic structure, so makers keep its resonance (fres ≈ c·VF / (2p), where p is the corrugation pitch) well above the operating band.
Why is corrugated cable lower loss than braided RG coax?
Three reasons. The seamless solid-tube outer conductor has no braid leakage and carries current over the full cross section, giving >120 dB shielding. Larger diameters (7/8", 1-5/8") cut conductor loss, which scales inversely with circumference. And the foam or air dielectric has εr ≈ 1.2 to 1.5 with loss tangent < 0.0003. Net result: 7/8" cable runs about 1.1 dB/100 ft at 1 GHz versus 6 to 9 dB for RG-213.
How do I calculate attenuation and power rating for a run?
Multiply the published α (dB/100 m) by length/100; attenuation rises roughly with √f below the dielectric-loss region. A 60 m run of 7/8" cable at 2 GHz (α ≈ 5.1 dB/100 m, scaled from 3.6 dB/100 m at 1 GHz) loses about 3.1 dB. Average power falls with frequency and ambient temperature (about 2.5 kW at 1 GHz, near 1 kW at 4 GHz for 7/8"), and you must derate for run VSWR and, with air dielectric, for altitude unless the line is pressurized.