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A
complete model of the Raibeam design must include a transmission
line with a given propagation delay, which is connected and
impedance matched to both of the driven elements. In this case,
small closed loops are used to accomplish the matching. Since there
is an inherent inability in NEC based modeling
programs to
accurately model small closed loops, inaccuracies arise when such
programs are used to
model this design.
One
can find a more than enough suggestions on how to deal with this
problem, but my experience has been that the inaccuracies remain,
regardless.
I have
also found found notable inconsistencies in both gain and impedance predictions
between differing NEC2d based modeling programs, including EZNEC+,
when modeling identical structures... interestingly, in comparisons between EZNEC+ and EZNEC Pro (NEC4)
the models proved to be
quite consistent. This leads me to conclude that NEC based modeling programs
can, and do,
produce artifacts. Granted, these compared programs were, in the
most part, unique to one another in how and in what form the output
information was presented.
Presentations
aside, perhaps a degree of these inconsistencies
are a product
of their theoretical basis; Maxwell's (classical) field theory.
Maxwell's
field point of view puts forward the idea
of local action-- where interactions of all kinds could be successfully
described as interactions happening at local points in space and
time, with the effects at other places being the result of propagating
fields. Thus, the generally accepted (classical) view is that electric
and magnetic fields are generated by RF energy being applied to an
antenna, and these fields then propagate to combine
in the far-field-- despite being out of phase-- to produce an electromagnetic
field which also propagates.
A
more modern view of electromagnetism holds that an electromagnetic
particle/wave (a photon) is produced by the perturbation of an
electron (by an alternating current, for example), and propagates
naturally without any need for the combining of electric and magnetic
fields in the far-field.
Further
arguments against the existence of electromagnetic fields was
put forth
by a prominent physicist; the late Nobel laureate Richard Feynman.
In his book QED*, Feynman states: "an effect
propagates from one point to another but this transmitted effect
lacks the physical reality of a field. This concept of a transmitted
effect is only a way of describing the literal action of one particle
on another at a distance. The idea of particles acting at a distance
on one another is a simpler, more satisfying description of electromagnetism
than the classical field theory which assigns substance to electric
and magnetic fields existing in space."
Setting aside the far-field issue, it appears there are other problems
with Maxwell's equations as well. For example, (the late) physicist John Wheeler, in his book
"Quantum Foam"
states: "Classical electromagnetic field theory does contain some notable
internal difficulties however. The worst of these difficulties is
the prediction that the field in the immediate vicinity of a point
particle is infinite in magnitude, resulting in "infinite self-energy"
of the particle, which seems to imply infinite mass. Interestingly,
this infinite self-energy can be swept under the rug - just ignored
- without disturbing the other successful predictions of the theory.
The difficulty is that when applied to quantum field theory this
infinite self-energy problem creates infinities."
It
seems logical to assume, then, that Maxwell's electromagnetic
field theory, while quite effective in its application for the most
part, is not entirely accurate. Granted, NEC based models of straight-forward
designs such as wire arrays, ground planes, dipoles, yagis, etc., and their
environments, are notably accurate. Nevertheless, it has been my
experience that the greater the complexity of the antenna, the greater
the chance of artifacts and resultant inaccuracies.
In
conclusion; regardless of the noted shortfalls, all NEC models
strongly suggest that the gain produced by the Raibeam's critical
coupling is indeed superior to that of an equal-length yagi. This
has been proven time and again by side-by-side and other on-air
comparisons.
*
Quantumelectrodynamics
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