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Shield effectiveness calculator — transfer impedance

Estimate how well a cable shield blocks interference: enter transfer impedance, cable length and the interference frequency, and read the shield effectiveness in dB.

Shield

Shield type

Typical transfer impedance Zt at 1 MHz — edit below for your datasheet value.

mΩ/m at 1 MHz — lower is better

Cable and interference

Metres of shielded cable in the run

MHz — the approximation holds best below ~1 MHz

Shield effectiveness

Shield voltage drop for 1 A
15mV
Shield effectiveness (SE)
16.48dB
Verdict
Weak

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Frequently asked questions

What is a good shield effectiveness in dB?

The calculator grades the result from the formula SE(dB) ≈ 20 × log10(100 / (Zt × L)) with Zt in mΩ/m and L in m. Below 20 dB is weak, 20–40 dB moderate, and above 40 dB good — a 1 mΩ/m shield over 1 m reads about 40 dB. Real braid coverage and aperture leakage often pull a high-frequency measurement several dB below the estimate.

What is transfer impedance and why is lower better?

Transfer impedance Zt is the voltage a 1 A interference current induces on the inner conductor across 1 m of shield — the figure of merit for a shield. Lower Zt means less noise couples in. Typical values at 1 MHz used here are about 10 mΩ/m for foil, 1.5 for 80% braid, 0.5 for 95% braid and 0.1 for solid shield.

How does cable length affect shielding?

Longer runs pick up more noise. The shield voltage drop for a 1 A noise current is V = Zt × L, so the coupled-noise reduction falls as length grows — doubling the length halves the shield effectiveness margin in the SE formula. Grounding strategy (one end for low frequency, both ends for RF) changes how well that shielding is realised.

How it works

Transfer impedance Zt is the figure of merit for a shield — lower is better. The shield voltage drop for a 1 A interference current is V = Zt × L, and the coupled-noise reduction follows SE(dB) ≈ 20·log10(100 / (Zt × L)) with Zt in mΩ/m and L in m. Braid coverage raises Zt at high frequency, and grounding both ends (for RF) behaves differently from one end (low-frequency) — the estimator here is an orientation, not a spec. IC Source Direct provides this tool for reference only.

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