For what it’s worth, my recollection is that the 1/r loss applies to an
infinite linear antenna. Thus it’s only an approximation for a real antenna.
As for evanescent waves, I have not seen a measurement of their speed of
initiation relative
to the distance to the source that generates them.
I don't think so. Electric fencers are relatively high voltage at 10Hz
AC. They are limited to very low current so you don't kill what touches
it. The 10Hz AC is very painful.
On Wed, Jul 20, 2016 at 5:47 PM, Jack Cole wrote:
> I thought this was very interesting. I
In reply to David Roberson's message of Wed, 20 Jul 2016 10:55:46 -0400:
Hi Dave,
Yes, I should have explicitly added that this is only valid where the separation
distance is <= the wavelength. Note however that because protons are massive
relative to electrons, and because the Earth's magnetic
The Air Conditioner That Makes Electricity
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I thought this was very interesting. I wonder what would happen to a
loaded electrolytic cathode or TiH2.
"Shrinking a quarter down to half its size sounds like a magic trick, but
there’s nothing magic about this experiment highlighted by Physics Girl
That's interesting! It is sort of complicated, like Rube Goldberg machine.
But so is a hybrid automobile. Sometimes complicated things work.
- Jed
too much envy in LENR land..
.
http://egooutpeters.blogspot.ro/2016/07/jul-20-2016-lenr-and-much-envy.html
Peter
--
Dr. Peter Gluck
Cluj, Romania
http://egooutpeters.blogspot.com
Robin,
It is my experience that the coupling falls off as 1/r to the third power at
large distances.
Dave
-Original Message-
From: mixent
To: vortex-l
Sent: Wed, Jul 20, 2016 12:04 am
Subject: Re: [Vo]:The principle of the mutual
That is correct. It even goes to 1/4th power at longer distances. The coil
are separated on air core RF transformers to increase the Q of the coils. This
leads to better selectivity/ tuning. The coupling does go down.
-Original Message-
From: David Roberson
I may be remembering wrong, but I believe that the evanescent magnetic
field strength falls off as 1/r^3 and the coupled evanescent power falls
off as 1/r^6. For the propagating field, the strength of the magnetic
field falls off as 1/r in free space and the coupled power falls off as
1/r^2. In
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