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Ham Radio 2000 #2
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Ham Radio 2000 - Volume 2.iso
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ANTENNA
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ELNECDEM
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ANTNOTES.DOC
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1991-02-01
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----- ELNEC Example Antenna File Notes -----
1 February 1991
Several example antenna description files are included on your
ELNEC disk. Following are some notes about each one. All files
have the extension ".EN" added to the name shown here.
Rather than having the examples all show ELNEC in its best light,
some were chosen specifically to illustrate weaknesses or
limitations you need to be aware of when using ELNEC or any
MININEC-based program.
DEMO USERS NOTE: The antennas marked '*' are too complex for the
DEMO program due to its 15-pulse limit, so they're not on the DEMO
disks. Also, some of the other antennas differ slightly from the
descriptions given here because the total number of segments was
reduced.
* 15MQUAD
The dimensions for this 15 meter quad, modeled in free space, come
from the ARRL ANTENNA BOOK, 15th ed., p. 12-2. The design is
attributed to W7ZQ. As it does on most quads, ELNEC (and MININEC)
reports a poor front/back ratio -- only 2 dB for this quad. This
is a result of MININEC's "cutting corners" where wires are
connected. A much more accurate analysis is obtained by tapering
the segment length using ELNEC's automated segment tapering
capability (see the manual for information). The result of
tapering is file 15MQUADT, described next. If you delete the
parasitic loop and look at the pattern of the driven element by
itself, you'll find that very few segments are necessary to obtain
an accurate pattern.
* 15MQUADT
If you take the 15 meter quad, above, and taper the segments using
ELNEC's automated segment tapering with default values, the result
is this model. The indicated front/back has improved to 8.3 dB
from 2 dB and the forward gain has increased about 0.8 dB. I
believe that this is an accurate representation of the operation of
this quad. You probably can get sufficiently accurate results with
fewer total segments by experimenting with the maximum and minimum
segment length when doing the tapering. Note that very many
segments per side are necessary to approach the accuracy of the
results achievable by using the segment tapering technique.
4SQUARE
This popular phased array was invented by Dana Atchley, W1CF. It
has several desirable properties. Because of its symmetry, it's
easy to switch in four directions. The forward lobe is broad
enough that four-direction switching gives good coverage to all
directions. Good rejection of signals occurs over a broad region
to the rear. The small rear nulls can be eliminated and the
forward gain increased slightly by increasing the element spacing.
However, this may make the physical spacing too far to conveniently
use some feed methods. Feeding of the four-square array is covered
in detail in Chapter 8 of the ARRL ANTENNA BOOK, 15th Edition. One
interesting feature of this array is that one element has a
negative feedpoint resistance if loss is low enough. This is a
valid result; the element is absorbing power from the others by
mutual coupling and feeding power back INTO the feed system. There
is still some lingering belief that the fields from the elements of
an array are proportional to the powers delivered to them. Element
1 of this array has a field equal to that from the other elements,
and it's FURNISHING power, showing the error in this belief.
Observing the currents in the elements reveals the truth: The
element CURRENTS determine the field strength, and they're equal in
all four elements.
CARDIOID
A popular phased array, the 90-degree phased, quarter-wavelength
spaced, two-element array is effective and forgiving, and gives an
honest 3 dB gain over a single element. It's modeled here over
perfect ground to point out the small reverse lobe which doesn't
usually show up in the textbooks. This is due to the change in
current distribution on the elements from mutual coupling effects.
See July 1990 QST, page 39, for more information on this phenomenon
and its consequences. For information on how to design a feed
system for this array see the ARRL ANTENNA BOOK, 15th Ed., Chapter
8, and "The Simplest Phased Array Feed System -- That Works" in the
second ARRL ANTENNA COMPENDIUM.
DIPOLE1
This is a plain dipole in free space, about the simplest antenna
you're likely to model. The frequency is 299.7+ MHz (selected by
entering '0' for the frequency), at which a wavelength is one
meter. The antenna dimensions, in meters, are therefore also the
dimensions in wavelengths. Note that this antenna, exactly a half-
wavelength long, is greater than a resonant length, as indicated by
the positive feedpoint reactance (seen by selecting 'SD' in the
Main Menu). A resonant "half-wave" antenna is somewhat shorter
than 0.5 wavelength, the amount depending on its diameter.
FDSP
A personal favorite, the "Field Day Special" has been built on
several bands and accounts well for itself from the home QTH as
well as on Field Day. It was described in June, 1984 QST. The
elements are folded dipoles made from twinlead, connected by a
half-twisted twinlead "phasing line". Folded dipoles are difficult
to model with ELNEC, so the elements are modeled as ordinary
dipoles with a diameter equivalent to the effective diameter of the
two-conductor twinlead. This is valid since the radiation
properties of ordinary and folded dipoles are identical -- only the
feedpoint impedance is affected by the "folding" process. The
program used to design the original antenna wasn't entirely
accurate so the element currents reported in QST weren't quite
correct. The source currents in the model are the currents
actually measured on the elements of a Field Day Special built to
the dimensions shown in the QST article. This antenna has a
respectable gain at low angles, a good f/b ratio, and a broad
forward lobe. It's also quite forgiving. Constructed from
twinlead, the input SWR is near unity.
* N4PCLOOP
This multiband horizontal loop antenna was created by Paul Carr,
N4PC, and described in December, 1990 CQ Magazine. A unique
feature is that it's driven at opposite corners by out-of-phase
signals as in the W8JK antenna. This results in an overhead null
on all bands. If you look at the Wires Menu description, you'll
see two sources shown IN phase. This is necessary due to a
combination of the way MININEC assigns pulses to wires and the
direction current is assumed to flow in the wires. When multiple
sources are placed in connected wires as done here, you must check
the resulting currents to make sure they're flowing in the
directions you thought. If not, you must reverse one or more
sources. Note also the relatively large number of segments for
each wire. On 20 meters, the 51-foot sides are approaching a full
wavelength long, so an appropriately large number of segments must
be used. See the manual for more information on multiband antennas
and on using multiple sources in an antenna.
NBSYAGI
This is a good test of program operation. The National Bureau of
Standards carefully built and measured several Yagi antennas. This
is a 50 MHz one, with dimensions from the ARRL ANTENNA BOOK, p. 18-
7.
VERT1
A "plain-vanilla" resonant vertical over average ground.
VERT2
Place VERT1 at the top of a 45-degree sloping hillside, and this is
what you get. Note the large improvement in low-angle radiation.
This is an example of use of the multiple ground media capability
of ELNEC. A linear boundary is used in this case.
W8JK
Originally designed by John Kraus, W8JK in about 1940, this antenna
has some interesting properties. It's characterized by two
closely-spaced elements driven out of phase. Although the fields
from the elements don't fully reinforce in any direction, gain is
nonetheless achieved because of lowering of the radiation
resistance due to mutual coupling. And lower it is -- note the
feedpoint impedance of only 3.73 - j24.48 ohms -- compare this to a
single element. The lower resistance results in heavier current,
hence greater field strength, for a given power input. The
difficulty is that system losses can quickly eat up the gain.
Making this antenna from #12 copper wire (try it -- and include
wire loss) drops the gain about 0.65 dB, not too bad. But great
attention must be paid to losses in matching networks. And losses
rapidly increase in significance as the spacing is made closer than
the 0.1 wavelength of the example. When mounted low (0.25
wavelength for the example), W8JK-type antennas have a lower
radiation angle than many other horizontal antennas due to the
inherent lack of high-angle radiation. As an interesting exercise,
save the pattern for later comparison. Then delete the second
source, making the antenna into a Yagi. Note the increased gain.
Even though the takeoff angle is higher, the Yagi gain is as good
or better even at lower angles. In addition, the feedpoint
impedance has increased to a much more manageable value. On the
other hand, the W8JK will retain its performance over a wide
frequency range, while the Yagi won't.