Richard,

Even though you are a "mechanical type," you have put your finger on a
week area in EMC design.  The brutal truth is that there are no good
design rules for shielding.  While this may be shocking, since it is far
from a new topic, it is due to the complexity of the problem.  If you
look at Maxwell's equations, they are difficult to solve analytically
for very simple geometries and impossible for realistic, real life
geometries.

Many of these published "rules" were developed more than a decade ago
(some three decades ago) and are based on a blend of theory and some
empirical data.  They all have a common flaw and work better in some
configurations than in others.  The common flaw is that they are based
on plane wave behavior (this means that you are in the far field) with
some corrections for being close in.  My experience is that you may
survey several sources of theory and either take the one that makes most
sense to you, or take portions of several to make your own composite
theory.  Here are some other sources:

1.      Reinaldo Perez, ed., Handbook of Electromagnetic Compatibility,
Academic Press, Inc., New York, 1995, pp. 401 - 443, ISBN 0-12-550710-0.
This is a chapter written by Richard B. Schulz.  Schulz's original IEEE
article is found in time #2 below.
2.      Schulz, R.B., et. al., "Shielding Theory and Practice," IEEE
Transactions on Electromagnetic Compatibility, 1968, EMC-10, pp. 168 -
175.  
3.      Violette, J, et. al., Electromagnetic Compatibility Handbook,
Van Nostrand Reinhold Co., NY,1987, ISBN 0-442-28903-0

If you are a real diehard, you may be interested to know that the EMC
Lab at University of Missouri - Rolla has been developing theory along
these lines.  Contact Dr. James L. Drewniak, 573-341-4969, or look up
their web site at http://www.emclab.umr.edu  Their approach may have
practical promise.  (They also have a good list of EMC books on their
site.)

To avoid the inaccuracies of the published theories on shielding (top
two paragraphs), many people have taken to numerical modeling of
specific problems.  With this approach, you solve these pesky Maxwell's
equations numerically, but this requires specific geometries and
produces results only appropriate to specific geometry addressed.
Finite Difference Time Domain (FDTD) is one of the more common types of
numerical techniques that are appropriate.  These also have some
well-known problems, but I will not bore you or the list-server with
those unless some one asks.

I am new in the computer industry.  Hence, I have asked myself these
same questions not too long ago.  My experience and the experience of
many colleagues in the industry that have spoken to is this:  if you
follow the guidelines based on classical theory that have been published
(the Schulz stuff is an example) you will usually overdesign.  These
methods drive you to very small vent holes and you equipment sounds like
a vacuum cleaner when forced air is used for cooling.

Good Luck,

Jim Knighten
------------------------------------------------------------------------
---------------------------
Dr. Jim Knighten
NCR
17095 Via del Campo
San Diego, CA 92127
Telephone: 619-485-2537
Fax: 619-485-3788
e-mail: [email protected]


        ----------
        From:  WOODS, RICHARD [SMTP:[email protected]]
        Sent:  Monday, July 20, 1998 5:57 AM
        To:  'emc-pstc'
        Subject:  Desiging Openings for EMC Compliance

        I am about to give a short seminar to our Mechanical Engineers
and Designers
        on enclosure design for EMC compliance. There is only one
problem - I have
        no faith in the theory I have for the attenuation through
openings. The
        following  formula is from the "EMC Handbook", Vol 3, by Don
White. Assuming
        the frequencies of interest are below the waveguide cutoff
frequency, the
        formula is 

                A(dB) = KL/G - 20 log N                 where,

                                K = 32 for round holes or 27 for square
holes
                                L = thickness of panel
                                G = hole diameter
                                N = number of holes.
         
        According to this formula, one 1/4 inch hole in a 0.090 inch
panel would
        have an attenuation of 11 dB, and  ten holes would have no
attenuation
        whatsoever. This does not match my experience in typical ITE.
Does anyone
        have any usable "rules of thumb" for Mechicanical types?
         
        Richard Woods
        Sensormatic Electronics
        [email protected]
        Views expressed by the author do not necessarily represent those
of
        Sensormatic.

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