Common-mode impedance coupling: Difference between revisions

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== Definition  ==
== 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&nbsp;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|R30}}). 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.


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All cables, including the protective conductors, have an impedance, particularly at high frequencies.


<br>[[Image:Fig R22.jpg|left]]<br><br><br><br><br><br><br><br><br><br><br><br><br><br><br><br><br><br>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>
{{FigImage|DB422796_EN|svg|R30|Definition of common-mode impedance coupling|


Current I2, present on the signal line, disturbs device 2. <br><br>'''''Fig. R32:''' 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>
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<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  ==


(see '''Fig. R33''')  
(see {{FigRef|R31}})  


*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.)
*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
*A common return path for a number of electrical sources


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{{FigImage|DB422797_EN|svg|R31|Example of common-mode impedance coupling}}
<br>[[Image:Fig_R23.jpg|left]]<br><br><br><br><br><br><br><br><br><br><br><br><br><br><br><br><br>
'''''Fig. R33:''' Example of common-mode impedance coupling''
 
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== Counter-measures  ==
== Counter-measures  ==


(see '''Fig. R34''')  
(see {{FigRef|R32}})  


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:  
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:
*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


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{{FigImage|DB422798_EN|svg|R32|Counter-measures of common-mode impedance coupling|
 
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.<br>
<br>[[Image:Fig R24.jpg|left]]<br><br><br><br><br><br><br><br><br><br><br><br><br><br><br><br><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. <br><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''
 
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[[ru:Гальваническая (кондуктивная) связь]]
[[zh:共模阻抗耦合]]

Latest revision as of 09:49, 22 June 2022

Definition

Two or more devices are interconnected by the power supply and communication cables (see Fig. R30). 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. R30 – Definition of common-mode impedance coupling

Examples

(see Fig. R31)

  • 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. R31 – Example of common-mode impedance coupling

Counter-measures

(see Fig. R32)

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. R32 – Counter-measures of common-mode impedance coupling
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