Oh, and the ferrite clamps have been deleted from CISPR 22 as part of
the latest FDIS and will not show up in CISPR 22:2005, which should be
published in the next few weeks.

The problem with the clamps is that they were not adequately defined and
you could still have different clamps, each meeting the 15 dB of loss in
50 ohms requirement, converging to different answers.

But, you are correct.  The NSA of an OATS or semi-anechoic chamber is
well defined, but how you get power to the EUT is totally open.  You
have no idea what sort of antenna you have (think of the power cord as a
random length, end fed antenna with an unknown termination at the far
end), so you have plenty of opportunities for variations in radiated
emissions from common mode currents flowing on the cord.  This applies
to any cable leaving the measurement area from table top equipment.  I
suspect this subject will arise again in CISPR SC I in the future, but
the earliest you might see an amendment would be 2008, and I wouldn't
hold my breath anticipating it to be that soon.

Ghery S. Pettit, NCE
Co-convenor, CISPR SC I WG3



From: [email protected]
[mailto:[email protected]] On Behalf Of Tim Williams
Sent: Tuesday, March 22, 2005 1:22 PM
To: [email protected]
Cc: [email protected]
Subject: Re: Radiated Emission Testing

The subject of non-repeatability in radiated emissions (and its lesser
brother,
non-repeatability in radiated immunity) provides perennial
entertainment. IMHO none of
the posts to date has put a finger on the number 1 source of
variability: cable
termination.

A 2m long cable is a quarter wavelength at 75MHz. If it is terminated to
the ground plane
with a low impedance then at this frequency it'll be a high impedance at
the EUT; vice
versa if it has a high impedance to the ground plane it'll be a low
impedance at the EUT.
Hence the radiated emissions due to a cable, typically below 200MHz as
Geetha has
described, will be directly related to the source impedance of the EUT,
the length of the
cable in wavelengths, and its far end termination impedance. S B Worm
did a very clear
paper a few years ago describing this experimentally and theoretically,
if anyone's
interested I'll dig out the reference. The work that has been ongoing on
the FAR method
for radiated emissions, and also the GTEM, has barfed on precisely this
problem.

None of the standards makes any attempt to control the termination
impedance. For as
long as this situation continues, variations between test houses will be
a fact of life. In
the test training courses that I run, it is incredibly easy to
demonstrate over 20dB
difference just through this one parameter. The ferrite clamps amendment
(A1 to
CISPR22:1998) did try to address the problem and was roundly condemned
by just
about all parties, each of which had their own set of interests to
defend. That being the
case, there is unlikely to be appreciable improvement in the near
future.

There are other factors of course: the OATS is conceivably the worst
possible test
method (in terms of repeatability) that could have been devised and
there are now better
methods, at least for small EUTs, easily available. Unfortunately they
all suffer from one
overwhelming disadvantage, which is that politically they are required
to show
correlation with measurements on an OATS, whose correlation with itself
is the subject
of such contention. This applies particularly for the FAR, the GTEM and
the reverb
chamber. I understand that some CISPR comittees are beginning to come
around to
the view that correlation between the results of different methods might
actually be
unachievable and so insisting on it would be a wasted effort. The light
at the end of the
tunnel?

Tim Williams
Elmac Services, Chichester, UK
http://www.elmac.co.uk


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