This is a multi-part message in MIME format.
Iain,
 
I have forwarded your question to Ed Hare of ARRL, below or attached is his
response.
 
Regards,
 
Dave Garnier
 


 
I can jump in, but this sure is a mess.
 
There are differences between "reactive" and "radiating" near field regions,
where one, essentially defined by lampda/2pi, there is E or H field field
strength, it is reactive in that energy is put into the field and then taken
back, with only a portion radiated.  There is the radiating field region,
where the fields are radiated, but one is not equidistant from all parts of
the antenna, so the relation between E and H vary over space, with non-planar
fields; standing waves of fields; varying phase relationships between E and H
and the probability that E/H will not be 377 ohms.
 
For a few examples:
 
http://p1k.arrl.org/~ehare/bpl/ppt/Hare_extrapolation_draft.ppt
 
I will correspond with him. 

Do either of you want to be cc's?

Ed Hare, W1RFI
ARRL Laboratory Manager
225 Main St
Newington, CT 06111
Tel: 860-594-0318
Internet: [email protected]
Web: http://www.arrl.org/
Member: ASC C63 EMC Committee
   Chairman: Subcommittee 5, Immunity
   Chairman: Ad hoc BPL Working Group
Member: IEEE P1775 BPL EMC Committee
Member: IEEE, Standards Association, Electromagnetic Compatibility Society
Member: IEEE SCC-28 RF Safety
Member: IEEE EMC Society Standards Development Committee
   Chairman, BPL Study Project
Member: Society of Automotive Engineers EMC/EMR Committee
Board of Directors: QRP Amateur Radio Club International 

 

  _____  

From: [email protected] [mailto:[email protected]] On Behalf Of Iain Summers
Sent: Wednesday, August 02, 2006 2:25 AM
To: [email protected]
Subject: Near field/Far field what is D.


There are various references and opinions as to what constitutes the near
field far field boundary. The common one from antenna theory is 2D^2/lambda
where D is defined as the largest aperture of the antenna. 
 
Has anyone researched what the limitations of this formula are? I am
interested in the far field boundary between 1-30MHz for large loops of wire.
In terms of a loop if this formula is applicable is D the circumference or
diameter of the loop.
 
Thanks,
Iain
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--- Begin Message ---
I can jump in, but this sure is a mess.

 

There are differences between "reactive" and "radiating" near field regions, 
where one, essentially defined by lampda/2pi, there is E or H field field 
strength, it is reactive in that energy is put into the field and then taken 
back, with only a portion radiated.  There is the radiating field region, where 
the fields are radiated, but one is not equidistant from all parts of the 
antenna, so the relation between E and H vary over space, with non-planar 
fields; standing waves of fields; varying phase relationships between E and H 
and the probability that E/H will not be 377 ohms.

 

For a few examples:

 

http://p1k.arrl.org/~ehare/bpl/ppt/Hare_extrapolation_draft.ppt

 

I will correspond with him. 



Do either of you want to be cc's?



Ed Hare, W1RFI

ARRL Laboratory Manager

225 Main St

Newington, CT 06111

Tel: 860-594-0318

Internet: [email protected]

Web: http://www.arrl.org/

Member: ASC C63 EMC Committee

   Chairman: Subcommittee 5, Immunity

   Chairman: Ad hoc BPL Working Group

Member: IEEE P1775 BPL EMC Committee

Member: IEEE, Standards Association, Electromagnetic Compatibility Society

Member: IEEE SCC-28 RF Safety

Member: IEEE EMC Society Standards Development Committee

   Chairman, BPL Study Project

Member: Society of Automotive Engineers EMC/EMR Committee

Board of Directors: QRP Amateur Radio Club International 



 





  _____  



From: [email protected] [mailto:[email protected]] 

Sent: Wednesday, August 02, 2006 10:24 AM

To: [email protected]; Hare, Ed W1RFI

Cc: [email protected]

Subject: RE: Near field/Far field what is D.





This is fantastic theory if you are doing this half way between the earth and 
the moon.  If not, you need to add the ground effect and a few other minor 
modifications into the formula due to wavelength, etc.  You also need to 
include wire-to-wire spacing, etc.  Wow.  Talk about over simplification.

 



Regards,



Wayne 

(302) TN633-8490 



 



  _____  



From: Garnier, David S (GE Healthcare) [mailto:[email protected]] 

Sent: Wednesday, August 02, 2006 10:06 AM

To: Hare, Ed W1RFI

Cc: [email protected]

Subject: FW: Near field/Far field what is D.





FYI - Maybe you would like to comment to the author

 

Note the reference to PLT

 

dave garnier

 





        David Garnier 

e GE Health Care 

___________________________________________ 



                David S. Garnier 

        Senior Technician 

        Functional & CT Engineering 

        3000 N. Grandview Ave - M/S W-1250 

        Waukesha, Wi. 53188 

        Tel: 262.312.7246 

        Cel:  414.899.7580 







  _____  



From: [email protected] [mailto:[email protected]] On Behalf Of Iain Summers

Sent: Wednesday, August 02, 2006 7:32 AM

To: [email protected]

Subject: Re: Near field/Far field what is D.





John thanks, 

 

I am aware that the boundary is a smooth transition and the main reason for 
wanting to know is to do with some subjective analysis of powerline 
telecommunications measurements that I have completed.

 

There are various papers that state that the attenuation of E with distance is 
1/distance(d) in the far field and some combination of 1/d, 1/d^2 and 1/d^3 in 
the near (or very near) field.

 

I have conducted measurements from 1-30MHz in a densely populated housing 
estate, in a semi rural college and at a semi rural house that has no objects 
to reflect the field strength back. I have plotted all of the graphs and 
included curves for 1/d^0.5, 1/d, 1/d^2, 1/d^3 and I am now in the process of 
correlating them. 

 

What I'd like to know is how large the measurement errors are. eg I have used a 
loop (which is the recognised method) and then converted to E for comparison to 
others results by using E/H=377 which is only true in the far field. I though 
it would be useful to determine what the results might be if E/H approached 
3000 or 30 say and for that  thought I'd use the point source formula 
lambda/2*pi and also 2*D^2/lambda to determine how near or far the boundary 
might be.

 

Sorry that is a bit of a ramble but that's the background to it.

 

You mentioned that D might be an area which was my initial thoughts as it is 
quoted for use as an aperture and therefore may not be wholly appropriate to 
use in the instance of the source being a large loop in the horizontal plane.

 

The overall aim of my PhD is not to come up with any answers per se but to 
explain to others who quote EMC theory in relation to PLT measurement. There 
are lots of assumptions but no one aver states "the answer is x and by the way 
that is + or - 50%". There are lots of people measuring E in dBuV to 2 decimal 
places with no mention of the errors in their measurements. This is fine for 
compliance if everyone does the same thing but some people are trying to 
predict interference based upon these results.

 

Thanks,

Iain  

 

 

 

----- Original Message ----- 

From: "John Woodgate" < <mailto:[email protected]> [email protected]>

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

Sent: Wednesday, August 02, 2006 8:59 AM

Subject: Re: Near field/Far field what is D.





In message < <mailto:001c01c6b604$c0ed2810$6401a8c0@homepc> 
001c01c6b604$c0ed2810$6401a8c0@homepc>, dated Wed, 2 Aug 

2006, Iain Summers < <mailto:[email protected]> 
[email protected]> writes

>There are various references and opinions as to what constitutes the 

>near field far field boundary. The common one from antenna theory is 

>2D^2/lambda where D is defined as the largest aperture of the antenna.



There isn't a sharp boundary. What you take as the boundary depends on 

why you want to know where it is, and you don't tell us that.



For example, you might decide that you want to know where the phase 

angle between E and H is only 1 degree. Or is 45 degrees. Or more.

> 

>Has anyone researched what the limitations of this formula are? I am 

>interested in the far field boundary between 1-30MHz for large loops of 

>wire.



Large compared with the wavelength at 1 MHz? That's large indeed!



>In terms of a loop if this formula is applicable is D the circumference 

>or diameter of the loop.



Or maybe the area?

-- 

OOO - Own Opinions Only. Try  <http://www.jmwa.demon.co.uk> 
www.jmwa.demon.co.uk and  <http://www.isce.org.uk> www.isce.org.uk

2006 is YMMVI- Your mileage may vary immensely.



John Woodgate, J M Woodgate and Associates, Rayleigh, Essex UK



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