Common-mode impedance coupling: Difference between revisions

From Electrical Installation Guide
m (1 revision: no page modification, previous revision = imported ch.R pages cleaned-up)
(Cleanup_2016)
Line 1: Line 1:
{{Menu_EMC_guidelines}}
{{Menu_EMC_guidelines}}
__TOC__
__TOC__


== Definition  ==
== Definition  ==


Two or more devices are interconnected by the power supply and communication cables (see {{FigRef|R32}}). 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.<br>All cables, including the protective conductors, have an impedance, particularly at high frequencies.
Two or more devices are interconnected by the power supply and communication cables (see {{FigRef|R32}}). 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.


[[File:Fig R22.jpg|none]]
All cables, including the protective conductors, have an impedance, particularly at high frequencies.
The exposed conductive parts (ECP) of devices 1 and 2 are connected to a common earthing terminal via connections with impedances Z1 and Z2.<br>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.<br><math>Z1\, I1=\left ( Zsign\, + Z2 \right )I2\Rightarrow \frac{I2}{I1}=\frac{Z1}{\left ( Zsign\, + Z2 \right )}</math> <br>


Current I2, present on the signal line, disturbs device 2. <br><br>'''''Fig. R32:''' Definition of common-mode impedance coupling''
{{FigImage|DB422796_EN|svg|R28|Definition of common-mode impedance coupling|
 
The exposed conductive parts (ECP) of devices 1 and 2 are connected to a common earthing terminal via connections with impedances Z1 and Z2. <br>
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.<br>
<math>Z1\, I1=\left ( Zsign\, + Z2 \right )I2\Rightarrow \frac{I2}{I1}=\frac{Z1}{\left ( Zsign\, + Z2 \right )}</math>  <br>
Current I2, present on the signal line, disturbs device 2.}}


== Examples  ==
== Examples  ==
Line 18: Line 23:
*A common return path for a number of electrical sources
*A common return path for a number of electrical sources


[[File:Fig_R23.jpg|none]]
{{FigImage|DB422797_EN|svg|R29|Example of common-mode impedance coupling}}
'''''Fig. R33:''' Example of common-mode impedance coupling''


== Counter-measures  ==
== Counter-measures  ==
Line 28: Line 32:


*Reduce impedances:
*Reduce impedances:
 
** Mesh the common references,
&nbsp; - Mesh the common references,<br>&nbsp; - Use short cables or flat braids which, for equal sizes, have a lower impedance than round cables,<br>&nbsp; - Install functional equipotential bonding between devices.  
**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
*Reduce the level of the disturbing currents by adding common-mode filtering and differential-mode inductors


[[File:Fig R24.jpg|none]]
{{FigImage|DB422798_EN|svg|R30|Counter-measures of common-mode impedance coupling|
If the impedance of the parallel earthing conductor PEC (Z&nbsp;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.<br>The difference in potential between devices 1 and 2 becomes very low and the disturbance acceptable. <br><br>
If the impedance of the parallel earthing conductor PEC (Z&nbsp;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.<br>
 
The difference in potential between devices 1 and 2 becomes very low and the disturbance acceptable. }}
'''''Fig. R34:''' Counter-measures of common-mode impedance coupling''


[[ru:Гальваническая (кондуктивная) связь]]
[[ru:Гальваническая (кондуктивная) связь]]
[[zh:共模阻抗耦合]]
[[zh:共模阻抗耦合]]

Revision as of 00:42, 14 December 2016


Definition

Two or more devices are interconnected by the power supply and communication cables (see Fig. R32). 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.

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. R28 – Definition of common-mode impedance coupling

Examples

(see Fig. R33)

  • 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. R29 – Example of common-mode impedance coupling

Counter-measures

(see Fig. R34)

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
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. R30 – Counter-measures of common-mode impedance coupling

ru:Гальваническая (кондуктивная) связь zh:共模阻抗耦合

Share