The elimination of the far field radiation pattern in plexciton radiation
by the Fano resonant interference is what makes the hot spot in
Nanophotonics so energetic, up to a 500,000,000 enhancement factor without
optimization.

Cheers:   Axil

On Sun, Mar 24, 2013 at 11:26 PM, David Roberson <dlrober...@aol.com> wrote:

> Harry, it is certainly true that the current flows in a loop.  The
> important issue is that each tiny portion of the loop radiates a signal as
> it accelerates, but that the integration of all of the individual signals
> balance out and results in no net radiation.   A circular loop of current
> will thus demonstrate a near field which is the magnetic moment of the
> loop, but does not generate a far field of radiation.  The near field
> component of the signal does not result in energy loss with time.
>
>  The motion of a single point charge does result in a far field radiation
> pattern since it accelerates along the circular path and does not have a
> balancing mechanism.  The trick is in the balance.
>
>  For the above reasons there would be no energy loss as a result of the
> current flow if it consisted of a continuous charge distribution orbiting a
> nucleus.  That is not true for a point charge following the same path.
>
>  Dave
>
>
> -----Original Message-----
> From: Harry Veeder <hveeder...@gmail.com>
> To: vortex-l <vortex-l@eskimo.com>
> Sent: Sun, Mar 24, 2013 10:28 pm
> Subject: Re: [Vo]:Re: CMNS: only a perfect LENR theory should attack other
> theories
>
>  On Sat, Mar 23, 2013 at 9:00 PM, David Roberson <dlrober...@aol.com> wrote:
> > Harry,
> >
> > An electron would not spiral into the nucleus if it is a continuous charge
> > instead of a point source.   Think of it as a steady DC current which
> > generates a magnetic field that does not radiate energy like an accelerated
> > charge.  This model is likely not correct, but it would achieve what you are
> > discussing.
> >
> > Dave
>
> All current flows in a loop so acceleration must occur in some zones
> in the loop.
>
> Harry
>
>
>

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