The distance of "one sixth lambda" comes from empirical data taken from a 
Hertzian dipole antenna.  In his book Introduction to Electromagnetic 
Compatibility ISBN 0-471-54927-4, Clayton Paul writes: "The point where the 
1/r3 (cubed) and 1/r2 (squared) terms become insignificant compared with the 
1/r terms is referred to the boundary between the near field and far field.  
This occurs where r = lambda/(2*pi).  The reader is cautioned that the boundary 
between the near and far fields for other antennas is not simply lambda/(2*pi), 
as is frequently assumed.  A more realistic choice for the boundary between the 
near and far fields will be discussed later, but can be summarized as being the 
larger of 3*lambda or 2*D*D/lambda, where D is the largest dimension of the 
antenna."  Simply stated, there exists some grey area between near and far 
field.  It depends on how closely your product resembles a Hertzian dipole.

Allen Tudor, Compliance Engineer
PairGain Technologies                  tel:  (919)875-3382
6531 Meridien Drive                         fax: (919)876-1817
Raleigh, NC  27616                           email:  [email protected]


>>> Meyerhoff Jerry-G10812 <[email protected]> 01/21 11:01 AM >>>

Hello group.
 
I substantially agree with the comments of Allen Tudor & 
Don Umbdenstock. My own view is :

I believe the 40 dB / decade (of distance) is a <questionable> approximation

for extrapolating the measurement antenna location being reduced from 10 
meter to 3 or possibly 1 meter in an effort to see the exceedingly weak 
emissions from well designed part 15 devices. However, below 30 MHz we're 
in the near-field of the source. 30 MHz is 10 meter wavelength and a 3 
(or 1 meter) meter antenna site spacing "violates" the accepted one sixth 
lambda near field to farfield transition zone. Some would argue that 1 
wavelength is a safer estimate of the transition zone. Then considering 
antennas like log periodics below 30 MHz which are huge, even that may 
not be large enough !! Or a 30 MHz (half-wave) dipole is 5 meters long . 
(as an aside.. How do you search 1 to 4 meters elevation in vertical 
polarization ?? (dig a hole for the lower dipole arm to fall into ;) <NOT> )
My personal rule is that the DUT to antenna spacing must be significantly 
greater than the antenna structure's max overall dimension to believe the 
outcome.  

Additionally , the 40dB approximation may have been derived from an
isotropic 
radiator in free space. I have a serious problem believing practical
antennas 
like dipoles, which have been calibrated & defined in the far field , can
give 
proper results when in a near field of any device being tested which may
have 
near fields dominated by either magnetic OR electric radiator effects OR a
strange 
and complex combination of both.  

I believe the "historical basis" of the part 15 method was defining VHF/UHF
TV's local 
oscillator unintended emissions (conducted to) its receiving antenna. We've 
extrapolated a long way from that simple 100 foot far-field antenna to
antenna 
coupling model.  

These comments are derived from (too) many hours of open field site
experience in measuring 
pt 15 on CB and 2 way VHF radios in the '70's and special CB to TV
interference studies 
with EIA TR-32 committee ~1976 when CB transitioned from 23 to 40 channels &
receiver 
emissions limits were reduced from 32 dBuV/m to ~ 10.. 

Hey this is way too much fun at work.
I have to get back to creating value for my customers. 

Best regards,
Jerry Meyerhoff
Principal Staff Engineer
Motorola AIEG [Automotive & Industrial Electronics Group] of
IESS [ Integrated Electronic Systems Sector ]
4000 Commercial Ave
Northbrook Il. 60062

DISCLAIMER:
This report represents the best opinions and analysis of the author
based on the information available which may be subject to change
without prior notice. The confidentiality of this info is everyone's
responsibility. Any opinions implied or expressed in this work are
solely those of the author . The suitability of this information for
making decisions rests solely with the reader. JDM :-)
1/21/2000





-----Original Message-----
From: [email protected] [mailto:[email protected]] 
Sent: Friday, January 21, 2000 5:50 AM
To: [email protected] 
Subject: Question on 15.31





I have not heard back fron the FCC on the following question. Does anyone
have any insight into the answer?

Thanks for your time,

Bob Heller

=============================
---------------------- Forwarded by Robert E. Heller/US-Corporate/3M/US on
01/21/2000 05:46 AM ---------------------------


Robert E. Heller
01/19/2000 09:52 AM
                                                    
      3M Product Safety,     St. Paul, MN 55107     
      76-1-01                                       
                                                    
      EMC Laboratory         Fax:  651-778-6252     
                                                    




To:   [email protected] 
cc:   Roger D. Kuhn/US-Corporate/3M/US
Subject:  Question on 15.31

Mr. LaForge, I have a question concerning paragraphs 15.31(f)(1) and
15.31(f)(2). Paragraph 15.31(f)(1) concerns measurements above 30 MHz and
at the bottom of the paragraph has a distance extrapolation factor of
20dB/decade. Paragraph 15.31(f)(2) concerns measurements below 30 MHz and
at the bottom of the paragraph has a distance extrapolation factor of
40dB/decade.

Why are there different extrapolation factors above and below 30 MHz?

Thank you,

Bob Heller
3M Company
651-778-6336
[email protected] 




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