Cable Impedance: Definition and Significance

Characteristic impedance is the resistance a transmission line presents to an electromagnetic wave propagating along it. Unlike DC resistance, which opposes steady current, impedance accounts for both resistive and reactive effects in AC circuits.

In practical terms, impedance mismatches cause signal reflections at junctions—connectors, terminations, or component interfaces. A reflection coefficient depends on the impedance ratio; even small mismatches degrade signal quality, introduce jitter, and reduce bandwidth. High-speed digital circuits, RF systems, and video distribution all demand precise impedance control.

Two cable families dominate:

  • Coaxial cables: Central conductor surrounded by a shield, separated by dielectric. Used in RF, video, and some data applications.
  • Twisted pairs: Two insulated wires twisted together, often in bundles. Standard for Ethernet, telephony, and differential signalling.

Impedance Formulas for Coaxial and Twisted-Pair Cables

The characteristic impedance of a transmission line depends on its inductance per unit length (L) and capacitance per unit length (C). For coaxial and twisted-pair geometries, closed-form expressions simplify calculation:

Coaxial cable:

Z₀ = (60 / √εᵣ) × ln(D / d)

Twisted pair:

Z₀ = (120 / √εᵣ) × ln(2S / D)

Propagation delay:

t = 84.72 × √εᵣ × 10⁻³ ns/m

Cutoff frequency (transverse EM mode):

f_c = 11.8 / (√εᵣ × 1000 × r_mean × π) GHz

  • Z₀ — Characteristic impedance in ohms
  • εᵣ — Relative permittivity (dielectric constant) of the insulation
  • D — Outer conductor inner diameter (coax) or wire-to-wire separation (twisted pair)
  • d — Inner conductor diameter (coax) or individual wire diameter (twisted pair)
  • S — Separation between wire centres in twisted pair
  • t — Propagation delay in nanoseconds per metre
  • r_mean — Mean radius of the transmission line cross-section

How to Use the Calculator

Select your cable type—coaxial or twisted pair—from the dropdown menu. The calculator automatically displays the required geometry parameters.

Enter the physical dimensions in millimetres or your preferred unit. For coaxial cables, provide the inner conductor diameter and the inner diameter of the outer shield. For twisted pairs, input the individual wire diameter and the centre-to-centre spacing between them.

The dielectric constant depends on the insulation material: typical polyethylene is around 2.25, polyimide approximately 3.5, and air-core cables approach 1.0. Leave this at the default value unless you have a datasheet specifying otherwise.

The calculator computes impedance, capacitance per metre, inductance per metre, propagation velocity, and the dominant-mode cutoff frequency. Use these results to verify component compatibility and signal propagation times in your circuit design.

Common Pitfalls and Design Considerations

Watch for these mistakes when working with transmission line impedance.

  1. Dielectric constant variability with frequency — The relative permittivity of an insulator is not truly constant—it varies with frequency, temperature, and manufacturing tolerances. Always check the cable manufacturer's specification sheet for the frequency range of interest. At high frequencies (GHz range), dissipation factors also become significant.
  2. Ignoring the entire transmission line — Impedance mismatch matters only if the cable length is comparable to or longer than the signal rise time (or wavelength at the signal frequency). Short stubs or patch cords on a logic board may tolerate poor impedance, but a 10-metre Ethernet run demands strict 100 Ω matching. Use the propagation delay to estimate round-trip transit time.
  3. Mixing measured and nominal dimensions — Manufacturing tolerance on cable diameter can be ±0.1–0.2 mm. Measure actual dimensions if precision matters—especially in high-speed systems. A 5% variance in diameter translates to roughly 10% change in impedance due to the logarithmic relationship.
  4. Overlooking launch and termination losses — Even a perfectly matched transmission line exhibits losses if connectors are corroded, solder joints are cold, or termination resistors have poor tolerances. High-frequency applications demand gold-plated contacts and 1% resistor tolerance.

Inductance and Capacitance Per Unit Length

The calculator also returns inductance (L) and capacitance (C) per unit length. These are useful for impedance verification and for computing characteristic impedance directly:

Z₀ = √(L / C)

For coaxial cables:

  • L = 5.08 × ln(D / d) µH/m
  • C = 1.41 × εᵣ / ln(D / d) pF/m

For twisted pairs:

  • L = 10.16 × ln(2S / D) µH/m
  • C = 0.7065 × εᵣ / ln(2S / D) pF/m

These parameters are essential for transient analysis, EMI filtering, and time-domain reflectometry (TDR) measurements. They also determine the cable's ability to support low-loss, high-bandwidth signalling.

Frequently Asked Questions

What is a good impedance for Ethernet cables?

Standard Ethernet cables (Cat5e, Cat6) are designed for 100 Ω differential impedance, measured between the two twisted pairs in a differential pair. This value was chosen to balance attenuation, crosstalk, and manufacturability at speeds up to 10 Gbit/s. Deviating from 100 Ω increases return loss and can corrupt data packets, particularly over longer runs (>50 m). Always verify cable impedance matches your network infrastructure.

How does cable length affect signal reflection?

Reflections occur at impedance discontinuities, not solely because of cable length. However, the electrical length of a cable determines whether reflected waves constructively or destructively interfere with the incident signal. If the cable length is much shorter than the signal wavelength (a fraction of the rise time), reflections may be negligible. At frequencies above a few hundred MHz, even 30 cm of mismatched cable can cause measurable degradation. Use the propagation delay to calculate round-trip time.

Can I measure cable impedance with a multimeter?

No. A standard multimeter measures DC resistance only, not characteristic impedance. To measure impedance, use a network analyser, impedance analyser, or a time-domain reflectometer (TDR). Some modern oscilloscopes have built-in TDR features. Alternatively, terminate the cable in its nominal impedance (50 Ω for RF, 100 Ω for Ethernet) and measure the insertion loss across the frequency range; impedance can be inferred from the S-parameters.

Why is 50 Ω standard for RF cables?

The 50 Ω standard emerged as a compromise in the 1960s. It minimises power losses in air-core transmission lines and offers good voltage-handling capability relative to loss. Modern coaxial cables with polyethylene dielectric achieve 50 Ω with reasonable outer conductor dimensions. For solid dielectric coaxes, achieving 50 Ω with small size is more difficult, so some applications use 75 Ω (video) instead. Always consult the component or system specification.

Does twisting tighter affect twisted-pair impedance?

Yes. Tighter twists increase the coupling between conductors, raising capacitance and lowering inductance. This generally decreases impedance slightly. The twist pitch (turns per metre) is therefore tightly controlled in Ethernet and other structured cabling standards. A typical Cat6 cable has a twist pitch of about 1–1.8 mm per pair to achieve and maintain 100 Ω impedance across its frequency range.

What happens if I use the wrong dielectric constant?

Impedance is inversely proportional to the square root of the dielectric constant. Using a value off by 10% causes impedance to shift by roughly 5%. Additionally, the propagation delay is directly proportional to √εᵣ, so errors cascade to signal timing predictions. Always obtain the dielectric constant from the cable datasheet or measure it via network analysis at the frequency of interest.

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