PS160L-110G-BF Phase Stable LD-PTFE RF Coaxial Cable

Cross-section structure diagram of PS160L-110G-BF LD-PTFE phase stable coaxial cable
Internal view showing silver-plated copper inner conductor, LD-PTFE dielectric, dual shielding, and blue FEP jacket.

PS160L-110G-BF

110 GHz Ultra-High Frequency Micro-Porous LD-PTFE Phase Stable Cable

Engineered for millimeter-wave testing and phase-critical RF environments, PS160L-110G-BF features a Micro-Porous Low-Density PTFE (LD-PTFE) dielectric. This advanced construction yields an impressive 76% velocity of propagation, significantly reduced attenuation, and exceptional phase stability under dynamic bending up to 110 GHz.

Max Frequency:DC-110GHz

Velocity of Prop.76%

Inner Conductor:Stranded SPC (1/0.3mm)

Outer Diameter:1.6mm

Structure & Construction Characteristics

LayerMaterialConstruction / Nom. O.D. (mm)
Inner ConductorSilver Plated Copper1 / 0.30 mm
Insulation (Dielectric)LD-PTFE (Low-Density PTFE)0.92 mm
Inner ShieldHelical Silver Plated Copper Strip1.05 mm
Outer ShieldSilver Plated Copper Wire Braid1.25 mm
Outer JacketBlue FEP1.60 mm
Min. Bending Radius (Static)8.0 mm
Min. Bending Radius (Dynamic)16.0 mm
Cable Weight0.006 kg/m

Electrical & Mechanical Characteristics

Impedance50 OhmCapacitance89 pF/m
Velocity of Propagation76%Max Operating Frequency110 GHz
Shielding Effectiveness> 90 dBDielectric Withstanding Voltage500 V @ DC
Phase Change vs. Bending±0.2 °/GHzPhase Change vs. Temperature≤ 1500 PPM (-45 to +85 ℃)

Attenuation & Power Handling @ 25℃ & Sea Level

Insertion Loss Formula: IL = K1 * sqrt(F_MHz) + K2 * F_MHz
Coefficients: K1 = 3.557846, K2 = 0.001221

Frequency (MHz)Nominal Attenuation (dB/100m)Max Power Handling (W @ 40℃)
30061.99150
50080.17116
1000113.7382
3000198.5347
6000282.9233
12000404.3923
18000499.3119
26500611.5315
40000760.4112
50000856.6111
670001002.739
1100001314.317

Model Comparison & Selection Note

Compared to our solid-PTFE variant (PS160L-110G-F), the PS160L-110G-BF utilizes an advanced Micro-Porous LD-PTFE dielectric. This provides a higher velocity of propagation (76% vs 70%), lower dielectric loss (attenuation reduced by ~14% at 18GHz), tighter phase stability vs bending (±0.2°/GHz vs ±0.3°/GHz), and an expanded operating temperature ceiling (up to +165℃).

Frequently Asked Questions

How does PS160L-110G-BF achieve higher propagation velocity than standard 160-size cables?

Operating up to 67 GHz requires avoiding higher-order waveguide modes within the coaxial structure. A 2.30mm outer diameter allows optimal dielectric dimensions (1.55mm) matching 1.85mm connector geometries, minimizing return loss and VSWR spikes at mmWave frequencies.

What is the main difference between PS160L-110G-BF and PS160L-110G-F?

 The “BF” suffix denotes a micro-porous LD-PTFE dielectric with enhanced temperature rating (-55 to +165℃) and lower attenuation, whereas the “F” suffix utilizes solid PTFE rated to +125℃.

What is the bend radius limit for installation?

The minimum static bend radius is 8.0 mm, while the dynamic bend radius for repeated flexure is 16.0 mm.

Need a Custom Solution?

To design the right custom RF coaxial cable, please share key details such as frequency range, application, required flexibility, installation space limitations, temperature requirements, and any existing cable model you are replacing. The more information you provide, the faster we can recommend the optimal cable solution.

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