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| Antenna Modeling |
From The Shack |
This
is a regular and popular monthly column by L.B. Cebik, W4RNL Because
computerized antenna modeling has become widespread, and its popularity as a design tool
continues to increase, this series is devoted to helping readers get the most from the
design software used. The articles focus upon the use of NEC and MININEC, along with
useful adjunct software as well. |
This column is primarily for "Guest
Editorials" to provide a podium for our readers to voice their opinions to the rest
of the world too. This is a chance for readers to get on their "soapbox" and
speak about antenna and radio-related subjects. Don't miss these interesting views about
anything and everything about radio and antenna systems! Now, what have YOU to say?? |
Ham WorkShop |
Stone's
Throw! |
|
Ham WorkShop, is also another
regular monthly column filled with a variety of "RADIO-STUFF" of value to
almost everyone in amateur radio from Novice to Extra and those just beginning to take up
this special hobby. This includes subjects, but not limited to: VHF, choosing the right
antenna, coax cable, small to mid-scale construction projects in a practical manner, use of test
equipment, etc. It is also meant to help readers become more familiar with the technical
jargon and the fun side of radio. |
Stone' Throw! a
monthly column by antenneX publisher,
Jack L. Stone, among other things, is to keep
the readers informed about our progress, new developments, plans for the future, and to
introduce the authors and their subjects each month. Also, our main slogan around here is
"we aim to please", so this serves as a place for the readers to tell the
publisher what is wanted or at least make suggestions. Just remember, the publisher is
only a Stone's Throw away! Go in for a visit and read this month's column. |
Propagation |
Propagation
another monthly column by Marcel H. De Canck, ON5AU of Belgium. Signal propagation
is a subject that is one of the most basic ingredients of radio and is something everyone
in radio should know about in order to maximize communications in the most effective way.
Its not enough to have the best equipment and the best antenna if you are trying to
send out a signal against a brick wall. Conversely, one may possess a very crude rig,
running low power, but yet transmit/receive a signal to great distances with ease, simply
by making use of a thorough knowledge about how signal propagation works within the
environment. Follow this column and learn more about propagation! |
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|
Forming Reasonable Expectations
of Modern Tri-Band Beam Designs
By L. B. Cebik, W4RNL
(A Posthumous
Publication) |
|
The most
modern tri-band beams for 20, 15, and 10 meters have given up traps
in favor of using individual elements for each band. Optibeam, Force
12, and Bencher all have beams based on this premise. Even for
relatively close total boom lengths, the element positions vary
considerably. The feed systems use either open-sleeve coupling or
direct-drive systems—or a combination of both. Compared to older
trap and hybrid designs, the newer beams present a somewhat
bewildering appearance, as if the boom were a porcupine on a
bad-hair day.
The somewhat confusing appearance presents many would-be users with
more than one quandary. Perhaps the most central is this question:
what should I reasonably expect by way of performance from these
beams? We are not wholly at the mercy of the manufacturer’s
specification sheets in forming our expectations. Instead, if we can
understand what goes into the design of such beams and can develop
an understanding of the performance of appropriately comparable
monoband beams, we can develop expectations that fit virtually any
of the newer designs. The goal of this set of notes is to go some
distance in this direction. |
|
Electromagnetic Fields of a
Small Helical Toroidal Antenna
By Kirk T. McDonald, PhD
Joseph Henry
Laboratories, Princeton University |
|
In these notes, we
shall discuss the electromagnetic fields of a helical toroidal
winding with major radius a and minor radius b, as shown below, that
carries is an oscillatory surface current that has no azimuthal
component. There is no accumulation of charge anywhere. It suffices
to consider the limit that we shall calculate where a
component is the wave number and c is the speed of
light.
A physical realization of this winding is shown as perhaps first
proposed by Corum where two counter windings of N/2 turns are
each driven with current such that the magnetic dipole moment is
zero. A complication in this case is that the N close
crossings of the two windings, there is localized, oscillating
charge accumulation due to the capacitance between the nearby wires,
which leads to azimuthal variation of the currents in the windings.
A solution follows which assumed sheet currents as stated above. We
first consider the static limit of sheet currents represented by
N terms of steady current with no azimuthal component. Then, the
electric field is zero everywhere, the magnetic field is zero
outside, the torus, while inside the torus we use Ampere's law (in
Gaussian units) to find the answer.
The fact that both static electric and magnetic vanish outside the
torus implies that all multiple moments vanished for a conventional
multipole expansion in this region. However, the vector potential is
certainly nonzero inside the torus, so that continuity of the vector
potential at its surface implies that the vector potential is
nonzero outside the torus as well.
To find the vector potential and the electric and magnetic fields in
the case of oscillating currents in the windings, we follow a method
due to Hertz. The electric and magnetic fields, E and B
can be derived from the scalar and vector potentials V and
A according to an equation in Gaussian units. |
|
Measurement of a High-Frequency
Current
By Igor Grigorov |
Radio Amateurs sometimes
give little attention to the need to measure HF current while
adjusting antennas, perhaps because an RF Ammeter that is both
affordable and adequate is not easy to come by.
In this paper, we will see that measuring RF current at HF is not
out of the reach to the average ham. In fact, it's possible to build
an RF Ammeter that is simple and accurate, opening up new horizons
of experimentation without being dependent on expensive lab
equipment. |
|
Transmission Lines
By
Ted Hart |
|
Every antenna book usually has a long detailed section on
transmission lines. You should read all that on a cold winter
evening when you have nothing better to do, or if you want to design
a special application antenna configuration. For simplicity, and
adequate information for the average amateur, all you really need to
know is a little bit about coax.
Sure, there are special applications for parallel conductor open
wire transmission lines, but they don't hook up directly to the coax
connector on the back of your rig. You need matching networks on
both ends and, if you don't really know all about those things, you
can't build a system that will use those techniques to advantage. |
|
Home-Brew Design and Construction
By L.B. Cebik, W4RNL (SK) |
|
Not every
amateur wishes to purchase equipment. Some amateurs prefer to build
rather than buy the basic equipment which goes into the shack. On
the chance that thoughts of this nature have entered your immediate
or future plans, we should look at some of the design and
construction features of home-brew equipment in at least enough
detail to permit some decisions. |
|
Transmission Line Theory
A Contribution From Academia
National Institute of Technology, India |
In an electronic
system, the delivery of power requires the connection of two wires
between the source and the load. At low frequencies, power is
considered to be delivered to the load through the wire.
In the microwave frequency region, power is considered to be in
electric and magnetic fields that are guided from lace to place by
some physical structure. Any physical structure that will guide an
electromagnetic wave place to place is called a Transmission Line. |
|
|

ARCHIVES Volume I, II, III, IV, V, VI,
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December 31, 2008
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