Precisely. The question is about the magnetic domain only. No need to introduce
voltage or 51.5 dB or near/far field. They are all totally irrelevant.
 
With best wishes DESIGN IT IN! OOO - Own Opinions Only
 <http://www.jmwa.demon.co.uk/> www.jmwa.demon.co.uk J M Woodgate and Associates
Rayleigh England
 
Sylvae in aeternum manent.
 
From: Ken Javor [mailto:[email protected]] 
Sent: Tuesday, February 28, 2017 4:11 AM
To: [email protected]
Subject: Re: [PSES] CORRECTION (wrong page) Passive Loop Emissions [General Use]
 
If we go all the way back to the OP:
The customer has requested an extended magnetic field emission test over the
range 100kHz to 2MHz with a limit defined in dBpT.
The antenna to be used is an EMCO 6512 which has it correction factors provided
in dBS/m which the emission software used does not recognise.
So is there a conversion factor that enables the right correction factor to be
entered or is the conversion factor only used once a result is obtained??

We can see that whether we are in the far field or not doesn't matter at all.

If we were using an electric field probe (say a 41" rod) to measure to a limit
expressed in dBuA/m or dBpT, then we would absolutely have to make an assumption
about the impedance of the wave in order to use a pure electric field
measurement to get at magnetic field characterization.

But that is not the case: we are using a shielded loop which not only inherently
measures the magnetic field, but rejects the electric field.  So we have a limit
expressed in units of magnetic flux density, which in air is directly
proportional to magnetic field (the 2 dB factor discussed previously) and we
have a loop antenna factor that gets us from the EMI receiver measured rf
potential to the magnetic field impinging on the loop that induced it.

Problem solved; case closed.

P.S.  For any who aren't convinced or don't follow the logic, look at the
antenna factors here:

http://www.ets-lindgren.com/charts/6512

Both factors are the same except for the 51.5 dB ohm offset, discussed
previously and both clearly exhibit the Faraday Law response of a loop to a
magnetic field as a function of increasing frequency. One can even derive the
loop inductance by looking at where the Faraday Law proportionality to frequency
flattens out: that is where the 50 ohm receiver impedance begins to load the
inductive output impedance of the loop.  It is not the magnetic antenna factor
that is in question; it is the electric field antenna factor that makes the
assumption of a plane wave. The magnetic field will be measured precisely; the
electric field measured using this loop is a guesstimate based on a far-field
assumption.

Ken Javor
Phone: (256) 650-5261



> From: Cortland Richmond <[email protected] <mailto:[email protected]> >
> Reply-To: <[email protected] <mailto:[email protected]> >
> Date: Mon, 27 Feb 2017 21:13:53 -0500
> To: <[email protected] <mailto:[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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