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. 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&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 '''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.  


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<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>
<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>


Current I2, present on the signal line, disturbs device 2. <br><br>'''''Fig. R22:''' 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''  


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== Examples  ==
== Examples  ==


(see '''Fig. R23''')  
(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.)
*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.)
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<br>[[Image:Fig_R23.jpg|left]]<br><br><br><br><br><br><br><br><br><br><br><br><br><br><br><br><br>
<br>[[Image:Fig_R23.jpg|left]]<br><br><br><br><br><br><br><br><br><br><br><br><br><br><br><br><br>
'''''Fig. R23:''' Example of common-mode impedance coupling''
'''''Fig. R33:''' Example of common-mode impedance coupling''


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== Counter-measures  ==
== Counter-measures  ==


(see '''Fig. R24''')  
(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:  
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:  
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<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>
<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>


'''''Fig. R24:''' Counter-measures of common-mode impedance coupling''  
'''''Fig. R34:''' Counter-measures of common-mode impedance coupling''  


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[[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 14:25, 19 October 2013

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.



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. R32: 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 R23.jpg


















Fig. R33: 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


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. R34: Counter-measures of common-mode impedance coupling



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

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