John, you ask why the difference in levels measured between test distances of 3 
meters and 10 meters. It’s fairly common for a device to fail at frequencies 
below 125 MHz at 3 Meter test distance and then pass at a 10 Meter test 
distance. Besides all the other possible factors (such as was a different 
chamber and test equipment used), the question becomes, was it a Near Field or 
Far Field RF signal that was being measured?  Near Field RF levels drop faster 
than Far Field RF Levels. The problem with a 3 Meter test distance is the 
frequency being measured might be impacted by Near Field, verses Far Field only 
measurement at 10 Meters. 

 

I have read a number of papers that claim different wave lengths for the Near 
Field effect. The values I have seen are between 1 and 3 wave lengths (with RF 
think wave lengths). I suspect it is system dependent and typically 1 to 2 
wavelengths and I suspect the primary reason for the effect between the two 
measurement distances. 

 

Here are the approximate possible frequency ranges impacted by Near Field at a 
test distance of 3 Meters: 

 

Three wavelength signal: RF levels up to 280 MHz 

Two wavelength signal: RF levels up to 140 MHz 

One wavelength signal: RF levels up to 70 MHz

 

As far as I am concerned 10 meters is the better test distance as it is in the 
Far Field for the frequencies between 30 MHz and 1 GHz. Although 30 Mhz is 
close to one wavelength at 10 Meters. 

 

 

Jim Bacher, WB8VSU

[email protected] <mailto:[email protected]>  or  [email protected] 
<mailto:[email protected]> 

 

From: John Woodgate <[email protected]> 
Sent: Wednesday, October 09, 2024 4:18 PM
To: [email protected]
Subject: [PSES] Technical musings

 

Reply to Derek @ LF Research, because his post is labelled as SPAM.

Yes, adding OATS is always healthy.😉

Is there an accepted explanation for the '3 m excess'? The published results 
are consistent with the field being diffuse (that term is from acoustics: I'm 
not sure how widely it's used in EMC circles), i.e the resultant of a large 
number of direct, reflected and diffracted rays. It is hardly surprising: a 
cuboid space is 'ideal' for producing a diffuse field above 'eigentone' 
wavelengths. This might create at least a 3 dB increase over 'inverse square' 
and maybe more. I suppose things get complicated at wavelengths that cannot be 
called 'short'.

Has anyone tried a spherical chamber? If that's too difficult, a 'quartic 
sphere [(x,y,z)^4 = r^4, like a Swedish traffic circle] has noticeably rounded 
corners and edges, so might be close enough for a useful improvement.

-- 
OOO - Own Opinions Only
Best Wishes
John Woodgate
Keep trying

 


 
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