[RFI] Inverse Square Law and RFI
Cortland Richmond
ka5s at earthlink.net
Wed Jun 13 12:15:38 EDT 2018
BPL was common mode for at least one horizontal conductor and (I don't
have access to the data) not a source, (arcing insulator, etc) local to
the pole/tower ground; at OUR frequencies; given the inductance of the
intra-pole ground conductor, the nearest vertical one *would* carry the
most RF current.
Cortland
KA5S
On 6/13/18 11:06 AM, JW wrote:
> Fortunately, Cortland , all of the power line noise sources I have had
> the pleasure to locate exhibited radiation from the vertical ground
> wire. Effectively, this represents a T-top loaded type vertical
> antenna with a pronounced vertical signal and signature.
>
>
> IT HAS been instructive, though TO NOTE the characteristics between
> signal bearings between say, two different disparate freqs like 400
> kHz and 1900 kHz versus 3.5 MHz
>
>
> I have found, during field work, the highest freq's bearing is THE
> correct one indicating the correct source when outside say 500 feet
> distance. For 400 kHz this can be nearfield of the vert ground wire,
> as well as saome radiation from a long horz line run.
>
>
> de Jim WB5WPA
>
>
>
>
> ------------------------------------------------------------------------
> *From:* Cortland Richmond <ka5s at earthlink.net>
> *To:* rfi at contesting.com
> *Sent:* Wednesday, June 13, 2018 9:11 AM
> *Subject:* Re: [RFI] Inverse Square Law and RFI
>
> This is an issue we lost in the BPL fight; when radiating conductors are
> long in wavelength, the transformation from near to far fields occurs
> at greater distance than would be expected of a point source. Ignoring
> radiator size (in wavelengths)-- part of the equation -- can result in
> substantially lower calculated interference potential from such sources.
>
> For 4 MHz
> (https://www.everythingrf.com/rf-calculators/antenna-near-field-distance-calculator
>
> ) and a 1000 meter radiating conductor:
>
> *
> Wavelength
> 74.9481145m
> *
> Reactive Near Field Distance
> 2264.70340834m
> *
> Radiating Near Field Distance
> 26685.12761585m
> *
> Far Field (Greater than this distance)
> 26685.12761585m
>
>
> Assuming a "point source" (ONE meter radiator)...
>
> *
> Reactive Near Field Distance
> 0.07161621m
> *
> Radiating Near Field Distance
> 0.02668513m
> *
> Far Field (Greater than this distance)
> 0.02668513m
>
>
>
> Cortland Richmond
> ka5s
>
>
>
> On 6/13/18 8:14 AM, JW via RFI wrote:
>
> > I suppose it should be mentioned, for completeness, that strictly
> speaking the inverse square law is inapplicable to that range of low
> band frequencies where propagation of the signal via ground wave is
> taking place, as on the 160 meter band,
> > de Jim WB5WPA
> >
> > From: Kenneth Goodwin <krgoodwin at comcast.net>
> > To: rfi at contesting.com
> > Sent: Tuesday, June 12, 2018 9:55 PM
> > Subject: Re: [RFI] Inverse Square Law and RFI
> >
> > The inverse square law is a geometric result based on the surface
> area of a
> > sphere that applies to an RF source radiating equally in all
> directions that
> > is in perfect environment, e.g. deep space. In most communication
> > environments the ratio is closer to the fourth power especially in
> far field
> > situations with all the good features of a typical RF environment -
> > scattering, diffraction, reflection, blockage, etc. Signal attenuation
> > depends on other factors like frequency not just the distance from
> the RF
> > source as stated in the inverse square law. As Jim has indicated in his
> > previous posting, in the real world it is never that simple. Ken K5RG
> >
> >
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>
> >
> >
> >
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