>“if you move a source towards / away from the antenna, the signal level should 
>follow the inverse square law – correct?”
>At most frequencies, the wavelength is long compared to the dimensions of the 
>shielded enclosure, so moving relative to the source is not done in a 
>far-field >condition and thus far-field relations don’t hold up.


IMHO, at most frequencies the wavelength is SMALL compared to the room, but at 
CRITICAL frequencies (<100 MHz) I agree with you Ed.
The boundary between close and far field is ( if I may refer to Henry Ott' 
works) around Lambda/2pi , so even with a  2-fold margin
the close-field/far-field boundary is extremely  small compared to the room 
(even if 3 of 5 meter).

>the distance between absorber and a reflective metal backing is important for 
>ensuring that the returning wave is in anti-phase”

It is recommended by several tile (ferrite) manufacturers to add a certain 
dielectric distance
between wall and ferrite tile, to shift the "resonance" frequency (the freq 
where incident and reflected wave "cancel")
down to a (desired) lower frequency at the cost of a slightly higher reflection 
coefficient.  Additional effect is a 
wider dampening bandwidth of the tile-wall combination . 
The optimum dielectric spacing is said to be tile thickness dependent.
Our FAR was built to this principle, and although I cannot compare (never build 
it without spacing)
it functions satisfactorily.  


Regards,

Ing. Gert Gremmen
Approvals manager
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From: Ed Price [mailto:edpr...@cox.net] 
Sent: Friday 29 April 2016 11:28
To: EMC-PSTC@LISTSERV.IEEE.ORG
Subject: Re: [PSES] Anechoic Chamber Questions

Jim:

“if you move a source towards / away from the antenna, the signal level should 
follow the inverse square law – correct?”
At most frequencies, the wavelength is long compared to the dimensions of the 
shielded enclosure, so moving relative to the source is not done in a far-field 
condition and thus far-field relations don’t hold up.

“the return loss characteristic gives the amount of absorption”
Yes, sort of. You may get some reflection from the front surface of the 
absorber. That’s a result of the absorber, but not exactly an absorption 
effect. The signal that does go through the absorber material then has to 
reflect off the shielded enclosure wall and then travel back through the 
absorber. So, the return signal has actually experienced two passes through the 
absorber and likely some scattering at the reflection. Still, it all adds up to 
a return loss. ☺

“with hybrid + tile absorber is it just a case of adding the return loss of the 
hybrid to the return loss of the tile”
Just moved past my level of experience, but I would expect that to not be true. 
I think you will see reflections due to mismatch at the absorber/tile 
interface, and this will affect the overall return loss. We need an expert to 
say how much.

“
The reflected signal will be shifted 180° by the massive impedance 
discontinuity (the metal wall), and I never heard of spacing the absorber off 
the reflective surface for any advantage. There will be some small phase 
shifting in propagation through the absorber, as the velocity of propagation 
will be different from air. I have heard of critical thickness and internal 
spacings for absorbers intended for stealth aircraft, but these are very 
frequency selective.

Paywalls are more like absorbers than reflectors, right?

Ed Price
WB6WSN
Chula Vista, CA USA

From: Pawson, James [mailto:james.paw...@echostar.com] 
Sent: Friday, April 29, 2016 12:14 AM
To: EMC-PSTC@LISTSERV.IEEE.ORG
Subject: [PSES] Anechoic Chamber Questions

Hello all,
 
I have some questions about anechoic chambers that I need some help with and 
I’m sure there is some expertise in this group that can help.
 
1. My understanding is that an anechoic chamber is meant to simulate a 
reflection-less, free space environment. Therefore if you move a source towards 
/ away from the antenna, the signal level should follow the inverse square law 
– correct?
 
2. When comparing absorber types (hybrid + ferrite tile vs. foam absorber) the 
return loss characteristic gives the amount of absorption at a particular 
frequency – correct?
 
3. If I wanted to compare effectiveness of foam absorber with hybrid + tile 
absorber is it just a case of adding the return loss of the hybrid to the 
return loss of the tile to achieve a final figure? My understanding is that the 
hybrid helps match the wave impedance from free space to that of the tile. Is 
the return loss of hybrid + tiles _together_ greater than the individual return 
losses of the separate components? Manufacturers that I’ve looked at list the 
data separately.
 
4. I have been told that the distance between absorber and a reflective metal 
backing is important for ensuring that the returning wave is in anti-phase (or 
at least as much as possible) with the incoming signal. However information on 
acceptable limits for this distance seems sporadic or in rarefied scientific 
papers behind paywalls. Does anyone have any info or experience on this point?
 
Many thanks for your time, I’m trying to get a handle on our chamber’s 
performance and any answers will help.
 
Regards,
James
 
 
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