4 ways in which noise can enter a signal cable and its control – Part 2

Electromagnetic induction and RFI

In previous part of this technical article, I wrote about electrical noise occurs or is transmitted into a signal cable system in the following four ways:

1. Galvanic (direct electrical contact) – part 1
2. Electrostatic coupling – part 1
3. Electromagnetic induction
4. Radio frequency interference (RFI)

3. Magnetic or inductive coupling

This depends on the rate of change of the noise current and the mutual inductance between the noise system and the signal wires.
Expressed slightly differently, the degree of noise induced by magnetic coupling will depend on the:

• Magnitude of the noise current
• Frequency of the noise current
• Area enclosed by the signal wires (through which the noise current magnetic flux cuts)
• Inverse of the distance from the disturbing noise source to the signal wires.

The effect of magnetic coupling is shown in Figure 1 below.

 

 

 

 

 

 

 

 

 

 

 

 

 

Figure 1 – Magnetic coupling

The easiest way of reducing the noise voltage caused by magnetic coupling is to twist the signal conductors. This results in lower noise due to the smaller area for each loop.

This means less magnetic flux to cut through the loop and consequently a lower induced noise voltage. In addition, the noise voltage that is induced in each loop tends to cancel out the noise voltages from the next sequential loop.

Hence an even number of loops will tend to have the noise voltages canceling each other out. It is assumed that the noise voltage is induced in equal magnitudes in each signal wire due to the twisting of the wires giving a similar separation distance from the noise voltage (see Figure 3).

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

Figure 3 – Twisting of wires to reduce magnetic coupling

 

 

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