Common-mode impedance coupling: Difference between revisions

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Definition

Two or more devices are interconnected by the power supply and communication cables (see Fig. R22). When external currents (lightning, fault currents, disturbances) flow via these common-mode impedances, an undesirable voltage appears between points A and B which are supposed to be equipotential. This stray voltage can disturb low-level or fast electronic circuits.
All cables, including the protective conductors, have an impedance, particularly at high frequencies.



Fig R22.jpg



















The exposed conductive parts (ECP) of devices 1 and 2 are connected to a common earthing terminal via connections with impedances Z1 and Z2.
The stray overvoltage flows to the earth via Z1. The potential of device 1 increases to Z1 I1. The difference in potential with device 2 (initial potential = 0) results in the appearance of current I2.
[math]\displaystyle{ Z1\, I1=\left ( Zsign\, + Z2 \right )I2\Rightarrow \frac{I2}{I1}=\frac{Z1}{\left ( Zsign\, + Z2 \right )} }[/math]

Current I2, present on the signal line, disturbs device 2.

Fig. R22: Definition of common-mode impedance coupling


Examples

(see Fig. R23)

  • Devices linked by a common reference conductor (e.g. PEN, PE) affected by fast or intense (di/dt) current variations (fault current, lightning strike, short-circuit, load changes, chopping circuits, harmonic currents, power factor correction capacitor banks, etc.)
  • A common return path for a number of electrical sources


Fig R23.jpg


















Fig. R23: Example of common-mode impedance coupling


Counter-measures

(see Fig. R24)

If they cannot be eliminated, common-mode impedances must at least be as low as possible. To reduce the effects of common-mode impedances, it is necessary to:

  • Reduce impedances:

  - Mesh the common references,
  - Use short cables or flat braids which, for equal sizes, have a lower impedance than round cables,
  - Install functional equipotential bonding between devices.

  • Reduce the level of the disturbing currents by adding common-mode filtering and differential-mode inductors


Fig R24.jpg



















If the impedance of the parallel earthing conductor PEC (Z sup) is very low compared to Z sign, most of the disturbing current flows via the PEC, i.e. not via the signal line as in the previous case.
The difference in potential between devices 1 and 2 becomes very low and the disturbance acceptable.

Fig. R24: Counter-measures of common-mode impedance coupling


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