Folks: The new antenneX
online issue #173 for the month of September 2011 is ready to read at your pleasure!
IN THIS ISSUE
We again include many fine articles by our global writing team. Now, please allow
me to introduce this month's line-up of content:
OUR MONTHLY COLUMNS:
- Antenna
Modeling By L. B. Cebik, W4RNL (SK)
This column has ended after
12 years, 3 months. 25 published posthumously.
Click here for more plans ahead
-
From the Shack
By Martin Steyer, DK7ZB
Traps with Toroidal Coils
In the
range up to 150 Watts RF Traps with toroid coils are simple to build and
to tune. A problem could be the parallel capacitor for high Voltage.
Experiments show in a load test that a Voltage of 2-2,5 KV for the C is
sufficient for proper working. If you cannot get such capacitors you can
use 4-5 C's with 500 V in series. In a test 3 x 100 pF/500 V in a
10-m-trap could handle 100 Watts. For the tests I used the toroid-types
T94-6, T94-2 and T106-2. The table shows the calculated number of turns,
in practice the real number is a little bit lower (nice for tuning...).
-
Antenna Design & Use
By
Justin Johnson, G0KSC
Stacking for beginners part 3
We have looked at the methods of connecting two
antennas together in quite some detail last month and also discussed the
types of antennas we should use as the basis of our stack. While the
intention was to get to modelling and configuring within EZNEC, we did
not quite get there! Therefore, this time we will work with EZNEC and
look how to establish the lengths our power splitters should be (using
this tool) in addition to using the functionality of EZNEC to easily
establish the best stacking distanced for our antennas.
-
Ham WorkShop
By Various Authors
Ham WorkShop, is also
another 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's Throw!
By Jack L. Stone, Publisher
A monthly column covering breaking news, new concepts and products,
people making news and introduction of the current month's issue articles and its
authorsalthough not limited to this only.
Dielectrically Loaded Antennas
NOTE: Starting earlier (in September 2010) and for the months ahead, there will
be an audio version of the main topic portion
of my column. It will be offered in two formats: 1)
Streaming for those with the “RealPlayer” media-type program
and, 2) MP3 for “MS Media Player” or similar programs. Links are
provided for both below:
It's been several years since the last audio version of my
column on the topic of the “antenneX mission.” In case you
haven't heard that one in 2006, here
it is:
Audio by Gary Nixon, WA6HZT
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FEATURE ARTICLES IN THE LIBRARY
OF NEW ISSUES:
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Adjustment
Sensitivity of Small 15-Meter Band Attic Antennas By
Grant Bingeman, P.E. KM5KG
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This article presents a simple and
effective method for tuning any antenna in the least amount of
time and with the least amount of frustration. An understanding
of antenna impedance behavior during the design phase is
developed using specific examples. This understanding will be
applied to the physical adjustment process during antenna
installation. The subject is a bit more complicated than might
at first appear to the casual antenna enthusiast. Therefore a
simple metric to quantify relative adjustment sensitivity is
presented so that the reader may compare antenna designs fairly.
Because an attic antenna is typically limited in size,
adjustment becomes more of an issue since 1) electrically small
antennas are more sensitive to their surroundings, and 2) a
small dimensional change can create large impedance changes. In
other words, electrically small antennas can be touchy, which
means their impedance changes rapidly.
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Practical Antennas: Part 4.05
By
Marcel H. De Canck, ON5AU
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The ionosphere
plays a tricky but an important role to our radio
communications, and there is very little we can do about it. But
there is plenty you can do about having a good and efficient
antenna system. Yes, antenna system, it’s not the antenna itself
but the whole part as transmission line, and matching properly
the transceiver and the antenna to the transmission line. It is
a breath-taking concept that a simple length of wire or rod or
tube can transform electrical energy into invisible radio
electro-magnetic waves that can cross the space at the speed of
light.
How does an antenna system works? Why does the
antenna radiate electro-magnetic waves? These questions I heard
many times and the answers are not given with few words.
Never-the-less, many books and some of great weight and
complexity have been written about antennas and many antenna
types have been developed and build. Often it is not
comprehensive to the layman to fully understand the whys and
hows of the radiation capabilities of an antenna and these
counts even for the simplest ones like a dipole or a
groundplane. Also I often hear many times misconceptions about
antenna properties and characteristics. To start with,
understanding why and how a simple antenna effective radiates
will be explained in a clear view. The dipole is the best
antenna to do that and once the secrets of the dipole
characteristics and properties are fully understood it will be
much easier to have a clear insight of the hows and whys of more
complicated antennas.
The first episodes will handle
completely about antenna fundamentals mostly with the half
wavelength dipole as study example. The dipole is also often a
part element of more complicated antennas such as a Yagi and
others. In particular for the low frequency bands, the dipole is
used by many radio amateurs as transmitting or receiving antenna
and its many practical installations and shapes will be fully
studied and explained in an episode later on. In fact many other
antenna types will become subject to explanation as the antenna
story develops.
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NewcomerNotes ~ Back to the
Basics: More Wire Antennas
By Robert Gulley, AK3Q
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Last month, in the August 2011
antenneX Issue #172, I took a look at wire antennas from a very
basic perspective: two wires forming a dipole antenna connected
to a feedline and cut to a specific frequency. I also discussed
some of the theory behind why these antennas work so well, and
why they can at times perform just as well as expensive
commercial antennas given the right conditions.
Wire
antennas represent one of the greatest values in the radio hobby
world. For less than the cost of a good meal out on the town you
can buy all of the necessary parts for a really good antenna,
and have change left over for a fast-food meal to boot!
This month I want to look at some more wire antenna designs, as
well as a bit more theory, while hopefully giving you some new
ideas for trying your own wire antenna setup. In addition to
being efficient and inexpensive, wire antennas have the added
bonus of being fun to build and to experiment with, since
mistakes are hardly costly and the materials are easy to work
with. |
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Simple
Building and Tuning of Traps
By Martin Steyer, DK7ZB
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Traps are useful for multiband
operating of all kinds of antennas. It is much easier to build
traps as you think and you do not need any special measuring
equipment for tuning. Only a transceiver each ham owns will be
needed and a simple homemade measuring circuit. A trap is a
parallel circuit of L and C on the frequency you want to close
an antenna segment. |
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THE MAGNETIC DIPOLE: A New
Theory for the Radiation Resistance of Ferrite Rod Antennas
By Alan Payne, G3RBJ
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A loop or coil can be used as an antenna, but the
received signal will be weak unless the coil is very large.
However the signal from a small coil can be enhanced
considerably by inserting a ferrite rod into it, because the rod
captures a volume of the incident electromagnetic field which is
much larger than itself, and concentrates this into the loop.
This capture effect is not unique — a conventional wire dipole
antenna also has an effective area vastly larger than its
physical area.
In the conventional theory this
enhancement when the ferrite is introduced is considered to be
due to the permeability of the rod (which is related to the
ferrite permeability), and so the ferrite antenna is seen as a
coil antenna with an enhanced effective area. However it is
shown later that this idea leads to an erroneous theory, because
the ferrite rod is in fact a magnetic dipole, and the coil
merely provides a means for detecting its flux. But we begin by
testing the accuracy of the conventional theory.
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Circular Nomograph for Converting
Between Field Intensity and Signal Level across the Antenna
Terminals By Harold Kinley, WA4GIB
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Before
describing how to use the nomograph, some background
information on the relationship between field intensity and the
signal level produced across the antenna terminals is in order.
Field intensity is the strength or intensity of the RF signal
level present at the antenna. The basic unit of measure of field
intensity is volts-per-meter (V/m). Generally speaking, the unit
of volts-per-meter is too large for most practical applications
so the terms microvolts-per-meter (µV/m) or millivolts-per-meter
(mV/m) are most often used to quantify the field intensity. A
field intensity of 1 µV/m is defined as the field intensity
required to produce a voltage of 1 µV across a wire 1 meter long
that is placed in an electric field with an intensity of 1 µV/m.
The wire is assumed to be properly oriented for maximum pickup.
Keep in mind that this discussion and the circular nomograph is
for a system impedance of 50Ω. |
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Hope you enjoy the new issue!
Jack L. Stone, Publisher
antenneX Online Magazine
http://www.antennex.com
jack@antennex.com
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