This a different issue. While the field strength outside a simple loop (a model 
for the EUT) falls off predictably (but  not as 1/r initially, as the field 
from the far side of the loop is not negligible), an EUT may require a much 
more complicated model, producing a field that falls off either more slowly or 
far faster than that of a simple loop.

I have studied this extensively for hearing loops, and I, and loop system 
manufacturers, have software to model the fields.

One thing to watch out for is that if you try to plot the field strength in a 
place with a reinforced concrete floor, the reinforcement greatly reduces the 
field strength so the results are not meaningful.

With best wishes DESIGN IT IN! OOO – Own Opinions Only
www.jmwa.demon.co.uk J M Woodgate and Associates Rayleigh England

Sylvae in aeternum manent.


-----Original Message-----
From: Cortland Richmond [mailto:[email protected]] 
Sent: Tuesday, February 28, 2017 2:14 AM
To: [email protected]
Subject: Re: [PSES] CORRECTION (wrong page) Passive Loop Emissions [General Use]

On 2/27/2017 7:53 PM, Brent DeWitt wrote:
> I think Ken's rational makes sense to me, since the 51.5 is derived from 
> 20*log(377).
>
>
Sure, but now we're back to how close we are -- wavelengths -- to the emitter. 
20*log(??)

Low frequencies can be tricky,  and I once had to double-check a test 
lab (not yours) results at a vendor, dragging the EUT out to their 
parking lot then wheeling a cart with a 6510 loop antenna, battery, AOR 
AR5000 receiver and RMS voltmeter [all mine] away to see  how fast the 
signal dropped with distance compared to 3m.

A fun time was NOT had, but I probably came across as a mad scientist. 
Again. At least no one ran out of a chamber...


Cortland Richmond KA5S

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