Crimping
How a Crimp Terminates a Coaxial Cable
A coaxial crimp termination is really two crimps performed in sequence. First the center pin is crimped onto the exposed center conductor using a small four-indent or hex cavity, forming the inner electrical path. Then a tubular ferrule is slid over the exposed braid and the connector body and compressed with a larger hex die, simultaneously clamping the braid for shielding continuity and gripping the cable jacket for mechanical strain relief. Because the process is purely mechanical, there is no heat-affected zone, no flux residue, and no risk of wicking solder up the braid and stiffening the cable, all of which are failure modes that plague hand soldering.
The joint integrity comes from cold flow. When the die compresses the soft copper or brass ferrule past its yield point, the metal flows plastically into the knurls or serrations of the connector body and into the interstices of the braid strands. The result is a large area of intimate metal-to-metal contact with the oxide layers fractured and excluded, which is what makes the joint gas-tight and stable over thousands of thermal cycles. The compression ratio, typically 15 to 25 percent reduction in ferrule outer diameter, is engineered so the metal yields without cracking the dielectric or shearing the braid.
Tooling discipline is the whole game. Production crews use ratcheting crimp tools that physically cannot release until the die reaches full closure, and the hex die size is dictated by the connector datasheet for one specific cable type. Mixing a die intended for RG-58 onto RG-142 will either under-crimp and let the connector pull off or over-crimp and crush the dielectric, ruining the impedance match.
Crimp Force and Compression Geometry
CR = (Dinitial − Dcrimped) / Dinitial × 100% (typ. 15 to 25%)
Hex Across-Flats vs. Diameter:
AF = Dcrimped × (√3 / 2) ≈ 0.866 × Dcrimped
Crimp Joint Resistance (parallel asperities):
Rc ≈ ρ / (2a) + ρfilm / (πa2) with Rc < 1 mΩ target
Required Crimp Force (approx.):
F ≈ σy × Acontact × k (k ≈ 2 to 3 for confined upset)
Where D = ferrule diameter, ρ = bulk resistivity, a = effective contact-spot radius, σy = ferrule yield strength, Acontact = crimped contact area, k = constraint factor. A 5.41 mm hex on annealed copper needs roughly 4 to 8 kN of press force.
Termination Method Comparison
| Method | Contact Resistance | Pull-out Force | Cycle Time | Frequency Limit | Best Use |
|---|---|---|---|---|---|
| Hex crimp | < 1 mΩ | 40 to 220 N | 5 to 15 s | ~18 GHz | High-volume cable assembly |
| Solder/clamp | < 0.5 mΩ | 90 to 250 N | 30 to 90 s | > 40 GHz | Precision and mmWave |
| Clamp (non-solder) | 1 to 3 mΩ | 110 to 200 N | 60 to 120 s | ~12 GHz | Field-installable, reusable |
| Compression (push-on) | 2 to 5 mΩ | 60 to 130 N | 10 to 20 s | ~3 GHz | CATV, fast field install |
| Twist-on | 5 to 20 mΩ | 20 to 60 N | 5 s | ~1 GHz | Low-cost consumer only |
Frequently Asked Questions
How do I choose the correct crimp die size for a coaxial cable?
Match the die callout on the connector datasheet to the matching tool cavity; it is dictated by the connector and cable, not chosen freely. RG-58 BNC uses a 0.213 in (5.41 mm) ferrule hex and a 0.068 in center-pin hex, while RG-142 and RG-400 use a 0.255 in ferrule hex. An oversized die under-crimps and lets the ferrule pull off; an undersized die crushes the dielectric and degrades return loss. Ratcheting tools enforce full closure to remove operator variability.
What pull-out force should a properly crimped RF connector withstand?
Miniature connectors on RG-58 and RG-174 should survive a 40 to 90 N (9 to 20 lbf) axial pull without separating, per MIL-STD-202 Method 211 and IEC 60352-2. Larger N-type and TNC on RG-213 run 110 to 220 N. The grip comes from the ferrule biting the braid and cold flow into the body knurls. Below-spec pulls usually mean an oversized die, missing braid under the ferrule, or a worn tool; lines verify on periodic sample coupons.
Why does crimping change the return loss of a coaxial connector?
A crimp alters local conductor and dielectric geometry, creating a small impedance discontinuity. Over-crimping compresses the dielectric and drops impedance below 50 Ω; under-crimping leaves an air gap that raises it. Either reflects energy, worsening return loss above 6 GHz where the crimp is an appreciable fraction of a wavelength. A controlled crimp holds better than 25 dB to 18 GHz, which is why mmWave assemblies favor captivated or solder contacts above 18 GHz.