HI all,

I have to agree with Ken, but what he says follows from his many years of
research and testing ( not saying you are old mate! ): he and I have similar
backgrounds. As we have all seen from the published documents from IEC, and
EN's, they are often done by folks who have never run a test: they are done
for repeatability more than anything.

The issue comes back to ( reluctantly ) what does the standard require to be
legally compliant. Some product standards recognise that a short cable will
just not couple energy from fields at lower frequencies ( Kudos to that
product committee ). Some product committees do not ( shame on them ).

If we only have the basic standard to work with, then we read the main body
and also informative notes. Just because they are not normative doesn't make
them not  applicable. The people that wrote the standards assume the users
will have some common sense and think about what they are doing to a test
item. If that's not being done, either train or replace the tester: simple.
EMC is not for the uninitiated.

My 5 cents worth.

Derek Walton

Ken Javor wrote on 2/26/2007, 11:34 AM: 

Regarding this: "I don't think we are testing efficiency of cable pick-up.  I
think we are testing immunity to whatever is picked up regardless of cable
efficiency."

I feel like Mr. Spock: "That is illogical."

A field impinges upon a cable.  An rf potential/current is coupled to that
cable. That coupled potential is a function of electrical length. The immunity
of the test sample to the coupled potential is then assessed.  The efficiency
of the coupling, or the transfer function, has to be accounted for.

The specific transfer function follows sin (2 p l/l) 

In case the symbols don't come through, that is

sin (2*pi*cable length/wavelength)

The RTCA/DO-160D/E and MIL-STD-461D/E conducted immunity limits follow this
equation asymptotically, using the peaks as the limit; the 1000-4-6 approach
was a fixed limit with a low frequency truncation.



From: Bill Owsley  <mailto:[email protected]> <[email protected]>
List-Post: [email protected]
Date: Mon, 26 Feb 2007 09:16:25 -0800 (PST)
To: Ken Javor  <mailto:[email protected]>
<[email protected]>, [email protected]
Subject: Re: Conducted immunity lower frequency






I don't think we are testing efficiency of cable pick-up.  I think we are
testing immunity to whatever is picked up regardless of cable efficiency.
 
If cable length and thus efficiency determined the lower cutoff frequency,
what is the formula to make a determination?  Is it a half wave, quarter wave,
1/5, 1/6, 1/10, 1/20 ?  to use some of the various "rules of thumb" for
relative efficiency.
 

 
- Bill
 


Ken Javor  <mailto:[email protected]> <[email protected]>
wrote:
 


I disagree with what I perceive is being stated here - that if any portion
of a system has a connection to a long conductor, then all system-attached
cables must be tested down to 150 kHz.

The purpose of the Annex B wording is to allow for basic physics to be
applied to the limit - short cables are inefficient pick-up at low
frequencies. It is the length of the individual cable-under-test which
should drive the low-frequency cut-off limit.

Ken Javor

> From: "Oliver Betz" 
> Date: Mon, 26 Feb 2007 11:30:21 +0100
> To: [email protected]
> Subject: Re: Conducted immunity lower frequency
> 
> Bob Richards wrote:
> 
>> Twice recently I've seen where annex B of 61000-4-6 ed2.2 is
>> referenced by someone and used as a reason for not requiring testing
>> down to 150 kHz "since the cable is specified as being less than x
>> meters in length". (Of course, this is after the EUT failed at a low
>> frequency!) 
> 
> Was Annex B applied correctly? Only very special setups are subject
> to higher starting frequencies, e.g. the keyboard attached to a
> battery powered PC, never used with AC adaptor.
> 
> Most devices are galvanically coupled to sources of low frequency
> disturbances, in this case the starting frequency must not be raised.
> 
> I read this from Annex B and it makes sense.
> 
> Oliver
> -- 
> Oliver Betz, Muenchen
> 
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