Ken,

 

I do not see any disagreement on the conversion of DM to CM, only
differences about what happens AFTER the conversion has happened.  

 

Then there are two possible views;

 

FIRST VIEW

This is the "What is on the Circuit diagram" view that is only valid at low
frequencies .  if I understand it properly, that is your argument and from
that position I agree with everything that you say, but consider further the
implications of the last sentence, repeated below;

 

It is only when the signal is referenced to ground that the radio receiver
becomes sensitized to it, because it has no line-to-ground filter elements
(Y-caps).

 

SECOND VIEW

The high-frequency radio engineer's view takes account of the transmission
line properties of the phase-to-neutral pair,  and also of the capacitance
to ground of the of the victim (radio in your example).

 

I affirm that;

 

-       Once the DM interference has been partly converted to CM - as we
have all agreed - then  that CM will be reflected back along the
phase-to-neutral pair towards the source in common-mode. That is the phase &
neutral are effectively in parallel and ground is the return path. 

Waves travelling along transmission lines are reflected at points of
mismatch.  This is how " Standing Waves" are produced and they are
well-known phenomena.  Since  CM current flow radiates - that was
unchallenged on the first day of this thread - the unbalanced mismatch at
the LISN will necessarily cause the radiation of interference FROM THE
INCOMING CABLE.  My original post did not mention LISNs.  I commented on the
real-world situation but it is much the same-or worse.

 

-       If we introduce to the scene a victim radio connected across the
phase-to-neutral pair, then the FIRST VIEW correctly says that the radio's
bulk cap does its job of filtering DM.  However, the radio sees the shift in
the reference level of the DM signal, because components of the radio have
some stray  capacitance to true ground.  The radio may be a very small box
on a wooden table, in which case that capacitance is only a few 10's of pF,
or it may be huge if the "radio" is a Hi-Fi radio with connection to a
roof-top antenna and to several loudspeakers.  This stray capacitance allows
the radio  to sense CM on its mains cable.  A "shift in the reference level
of the DM signal"  is another way of saying "CM"  and so that now has the
capability of creating interference if the receiver design is inadequate.
There are many ways for stray currents to get into low-level analogue
circuitry.  I did not mention radios either: the analysis is valid across
the board. 

 

So it is the circuit components that are not on the equipment circuit or on
its cabling layout that matter at Radio Frequencies - and that is where EMC
gets seriously interesting.

 

Richard

 

Richard Marshall Laboratories,

30 Ox Lane, Harpenden, Herts.,    AL5 4HE, UK 

+44 (0)1582 460815      <http://www.design-emc.co.uk> www.design-emc.co.uk

Member of the EMC Industry Association

 

From: Ken Javor [mailto:[email protected]] 
Sent: 03 April 2016 17:48
To: [email protected]
Subject: Re: [PSES] Common mode current vs. differential mode current and
LISN

 

I think there is a fundamental misunderstanding of the mechanism converting
dm into cm, both on the part of Michel Mardiguian back in the day and those
who repeat his criticism in this thread.

What people are saying, (if I understand it properly) is no different than
if I used two LISNs, one with a different inductor value than the other.  In
that case, at frequencies where at least one LISN did not look like 50 ohms,
the EMI port measurement for the dm part would be different on each LISN,
and that would make it look like a cm signal, and therefore we have a
problem.

But that is flatly incorrect. The issue is not the relative value of the dm
portion at each LISN, but rather the reference for the signal.  For dm,
regardless of "balance" both dm LISN contributions sum and they are
referenced from phase-to-neutral, not conductor-to-ground.  As long as the
dm contributions are phase-to-neutral, the bulk cap in the victim radio
power supply does its job of filtering and doesn't care how much dm is
measured to ground at each LISN.  It is only when the signal is referenced
to ground that the radio receiver becomes sensitized to it, because it has
no line-to-ground filter elements (Y-caps).

This point was made abundantly clear in the report that was presented to
TC77 back in 1998 (or thereabouts).

Ken Javor
Phone: (256) 650-5261



  _____  

From: Richard Marshall < <mailto:[email protected]>
[email protected]>
Reply-To: Richard Marshall < <mailto:[email protected]>
[email protected]>
Date: Sun, 3 Apr 2016 12:54:43 +0100
To: < <mailto:[email protected]> [email protected]>
Subject: Re: [PSES] Commom mode current vs. differential mode current and
LISN

Rich
 
I'm sorry!
 
 I did notice the X when it should have been Y when I received my list copy.
I decided to wait to see who was alert enough to correct me.
Well done and Thank you.
 
The usual class Y value of 4,700pF presents an impedance of only 1.13 ohms
at 30MHz, so it provides a very substantial unbalance to create CM from a
neighbour's DM
 
 

Richard
 
Richard Marshall Laboratories,
30 Ox Lane, Harpenden, Herts.,    AL5 4HE, UK 
+44 (0)1582 460815      <http://www.design-emc.co.uk> www.design-emc.co.uk
<http://www.design-emc.co.uk> <http://www.design-emc.co.uk> 
Member of the EMC Industry Association
 

From: Richard Nute [ <mailto:[email protected]]> mailto:[email protected]] 
Sent: 02 April 2016 18:24
To:  <mailto:[email protected]> [email protected]
Subject: Re: [PSES] Commom mode current vs. differential mode current and
LISN

 


-       A device with a single class X capacitor from neutral to ground.


Safety standards require the capacitor to be Class Y.
 
 
Rich
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