qex-ground-systems-part-5.pdf

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Rudy Severns, N6LF
PO Box 589, Cottage Grove, OR 97424; n6lf@arrl.net
Experimental Determination of
Ground System Performance for
HF Verticals
Part 5
160 Meter Vertical Ground System
How much will the signal strength and feed point
impedance change as radials are added?
This experiment was actually the irst
of the series of experiments on ground
systems that have been the subject of this
series of articles. The experiment involved
measuring the change in signal strength as
radials are added to the ground system of a
vertical antenna, beginning with four radials
and going up to 64 radials. The intent was
to determine the additional gain in signal
for each doubling of radial number, and to
determine the point of vanishing returns. In
addition, the changes in feed point imped-
ance due to changing radial number were
of interest.
While the results of this initial experiment
were quite interesting, a more important
result was an appreciation of the dificulties
of making these measurements accurately.
This experience led to a modiication in the
test procedure and a shift to 40 m verticals,
which have been described earlier.
Figure 1 — This photo shows the antenna base with radials attached.
Test Antenna Description
The test frequency for this experiment
was 1.800 to 2.000 MHz. The vertical was
125 feet of no. 12 AWG insulated copper
wire suspended from a Dacron line hung
between two 150 foot poles.
At the base of the antenna there was an
18 inch diameter copper disk, as shown in
Figure 1. The inner ends of the radials and
The terrain around the antenna was not
lat, but rather on a narrow ridge about 40
to 50 feet wide. The result is that many of
the radials were in part bent down at about
a 45° angle as they ran down the steep slope
on either side. Along the ridge, however, the
radials are more or less level.
the shield of the coax feed line were attached
to the disk. There were also two galvanized
5 8 inch × 4 foot ground stakes connected to
the disk. The radials were 130 foot lengths of
no. 12 insulated (THHW) wire lying on the
ground surface. Radials were put down in
the sequence of 4, 8, 16, 32 and 64.
QEX – July/August 2009 15
989409778.038.png 989409778.039.png
The test antenna was erected 700 feet
to the east of my house with a 50 foot deep
gully in between. The ridge is in a Douglas ir
forest with 100 plus foot trees within 50 feet
of the test antenna at some points. The radial
system ran along the ridge and also down the
sides of the ridge into the forest.
To excite the test antenna, between the
house and the antenna there was a 700 foot
length of 1 5 8 inch coax, with an additional
75 feet of ½ inch coax. Both were Andrews
heliax.
Table 1
Typical Test Data for Received Signal Strength with P o = 50 W.
Number of Radials
Corrected Signal Strength
Relative Signal Strength
4
–30.1 dBm
0.0 dBm
8
–29.3 dBm
0.8 dBm
16
–28.9 dBm
1.2 dBm
32
–28.0 dBm
2.1 dBm
64
–27.7 dBm
2.4 dBm
2.5
Measurement Equipment
The signal source was a Yaesu FT1000MP
transceiver with two Bird Model 43 wattme-
ters on the output (forward and reflected
power). The wattmeters were used to set the
forward power to a constant 50 W and also to
measure relected power to calculate SWR.
The SWR measurement is needed to correct
for the power relected from the antenna and
not radiated. This correction was applied to
the received signal amplitude.
The receiving antenna was a 10 foot
vertical wire driven against a 4 foot ground
stake, next to my house. The receiver was an
HP3585A spectrum analyzer. The amplitude
resolution was about ± 0.1 dB.
Base impedance measurements were
made at the antenna using an N2PK vector
network analyzer (VNA). The impedance
measurements were accurate to better than
1%.
The test procedure was very straight-
forward. For each number of radials, the
FT1000MP output was adjusted to 50 W and
received signal strength on the spectrum ana-
lyzer recorded along with the SWR for that
measurement and the input impedance at the
base of the antenna.
2.0
1.5
1.0
0.5
160 m Te st Vertical
August 2006
Run 2
0.0
4
8
12
16
20
24
28
32
36
40
44
48
52
56
60
64
Number of Radials
QX0907-Severns2
Figure 2 — Here is a graph of the typical signal strength change with radial number.
70
4 Radials
160 m Test Vertical
August 2006
Run 2
65
8 Radials
Test Results
Three complete runs were made to verify
repeatability of the measurements. Each run
included a complete stepping through the
number of radials in the sequence, 4, 8, 16,
32 and 64. Typical received (and corrected
for SWR) signal strengths versus radial num-
ber are given in Table 1. This data is graphed
in Figure 2.
The data in Figure 2 has one obvious odd-
ity. You would expect that the incremental
difference as the radial numbers are doubled
would be monotonically decreasing as the
radial number rises. The step between 16
and 32 radials does not do this and it appears
that the value for 16 radials is too small. This
anomaly was noted during the experiment,
however, and checked carefully as the radial
count was redone three times. The anomaly
was there in all three cases. I have no expla-
nation for this other than the irregularity of
60
16 Radials
55
32 Radials
50
64 Radials
45
40
35
1.80
1.82
1.84
1.86
1.88
1.90
1.92
1.94
1.96
1.98
2.00
Frequency (MHz)
QX0907-Severns3
Figure 3— This graph gives the resistive part of the base impedance over the 160 m band for
different radial numbers.
16 QEX – July/August 2009
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the site, which forced the radial layout to
be far from lat or level. Later experiments
with more regular radial systems on other
antennas all showed the expected monotonic
decrease in improvement with increasing
radial number.
In any case, it’s pretty clear that 32 radi-
als do a good job and by 64 radials you are
well into the region of vanishing returns. I
certainly could not justify doubling the radial
count to 128!
The results of feed-point impedance mea-
surements are given in Figures 3, 4 and 5.
As discussed in Part 2 of this series, we
would expect the resonant frequency to vary
with the number of radials, due to the shift in
radial resonance because of soil loading. The
40 m experimental work was done over an
essentially lat pasture and the resonant fre-
quency change was regular and monotonic.
The gross irregularity of the ground surface
in this earlier experiment, however, resulted
in the erratic frequency changes shown in
Figure 5. This problem was a primary reason
for moving the experimental site from the
narrow ridge to a pasture. Unfortunately, the
150 foot support poles were not available in
the pasture so it was necessary to change the
experimental frequency to 40 m to make the
vertical height manageable.
65
160 m Te st Vertical
August 2006
Run 2
1.9 MHz
60
55
50
45
40
4
8
12
16
20
24
28
32
36
40
44
48
52
56
60
64
Number of Radials
QX0907-Severns4
Figure 4 —This graph shows the base resistive component versus radial number at 1.9 MHz.
1.920
160 m Te st Vertical
August 2006
Run 2
1.915
Summary
This initial experiment helped me to
understand the problems inherent in mak-
ing accurate comparisons between different
ground systems. I had to change the site,
the test frequency, the test instrumentation
and the test methodology to get to the point
where I could have conidence in the test
results and draw conclusions from them.
This experiment was by no means a fail-
ure, however. We can see that the change
in signal strength is very much in line with
what we saw in the 40 m work. It also sup-
ports the conclusion that we should use at
least 16 radials, but when we use more than
32 radials we are definitely reaching the
point of vanishing returns. For most amateur
installations the Standard Broadcast ground
system of one hundred twenty 0.4-wave-
length radials could not be justiied by any
useful increase in signal strength.
1.910
1.905
1.900
1.895
4
8
12
16
20
24
28
32
36
40
44
48
52
56
60
64
Number of Radials
QX0907-Severns5
Figure 5 — This graph shows the antenna resonant frequency for different numbers of
radials.
Rudy Severns, N6LF, was irst licensed as
WN7WAG in 1954 and has held an Extra class
license since 1959. He is a consultant in the
design of power electronics, magnetic compo-
nents and power-conversion equipment. Rudy
holds a BSE degree from the University of
California at Los Angeles. He is the author of
two books and over 80 technical papers. Rudy
is an ARRL Member, and also an IEEE Fellow.
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