Lesson 5/1050%
MODULE 05

LISN, EMI Receiver & Test Setup

Two pieces of equipment make conducted-emission testing possible: the LISN, which isolates the EUT from mains noise and diverts a calibrated fraction of the EUT's own noise into a measurement port, and the EMI receiver, which sweeps that signal across frequency. This module opens both up and shows how a full test bench comes together.

A LISN (Line Impedance Stabilization Network) does two jobs at once: it presents a fixed, standardized impedance to the EUT so measurements are repeatable across labs, and it diverts a defined fraction of the EUT's noise current into a calibrated 50 Ω port feeding the receiver — while blocking noise coming from the mains supply itself from contaminating the measurement.

Animated: LISN Equivalent Circuit

The blocking inductor stops mains-side noise from reaching the EUT and forces EUT-generated noise to flow toward the 50 Ω measurement port instead of back into the mains. The path currently carrying signal is highlighted.

Component Typical Value Purpose
Blocking inductor (L) 50 µH (per CISPR 16-1-2) Blocks mains-side noise; forces EUT noise toward the measurement port
Coupling capacitor ~0.1–8 µF Couples the EUT's noise current into the 50 Ω measurement path
Measurement resistor 50 Ω Provides the calibrated impedance the EMI receiver expects
Termination resistor (unused port) 50 Ω Terminates the port not currently feeding the receiver, so it doesn't distort the measurement

Click each control below to see what it does on a live sweep.

A repeatable CE test needs more than a LISN and receiver: the EUT sits on an insulated table above a bonded ground plane, is fed through an isolation transformer to keep facility mains noise out of the measurement, and every metal enclosure on the bench is bonded to the same ground reference.

LISN
EMI Receiver
Ground Plane
Isolation Transformer
Power Source
EUT
Non-Conductive Table
Bonding Strap
Cable routing matters: standards typically specify cable bundle length above the ground plane (often ~80–100 cm), height above the plane (a few cm), and distance from the LISN to the EUT — changing any of these can shift the measured spectrum, especially at higher conducted frequencies where cable resonances start to matter.
KNOWLEDGE CHECK

Module 5 Quiz

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