[TowerTalk] W0IYH Feed line Choke Performance
Joe Subich, K4IK
k4ik at subich.com
Tue Aug 19 16:20:04 EDT 2003
Here is the WA2SRQ data from my personal archive ...
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Having access to a Hewlett-Packard 4193A vector impedance meter at work,
I have made measurements on a number of baluns, coaxial and otherwise.
For my beams I was particularly interested how many turns and on what
diameter are optimum for air core coaxial baluns, and what the effect of
bunching the turns was (formless). Using the remote programming capability
of the HP4193A along with an instrument controller, I measured the magnitude
and phase of each balun's winding impedance at 1 MHz intervals from 1 to 35
MHz. For comparison, I also made measurements on a commercial balun which
consists of a number of ferrite beads slipped over a short length of coax.
I've appended some of these measurements so you can draw your own
conclusions.
PVC pipe was used for coil forms. The 4-1/4 inch diameter baluns were wound
on thin-walled PVC labeled "4 inch sewer pipe". This material makes an
excellent balun form. It's very light weight and easy to work with, and I
obtained a 10 foot length at the local Home Depot for about 3 dollars. The
6-5/8 inch diameter forms are 6 inch schedule 40 PVC pipe which is much
thicker, heavier, and more expensive.
Each test choke was close-wound on a form as a single-layer solenoid using
RG-213 and taped to hold the turns in place. The lengths of cable were cut
so there was about 2 inches excess at each end. This allowed just enough
wire at the ends for connections to the HP4193A's probe tip. After data was
collected for each single-layer configuration, the PVC form was removed, the
turns were bunched together and taped formless, and another set of
measurements
was taken. I have only included the "bunched" measurements in the table for
one of the baluns, but the trend was the same in each case. When compared
to
the single-layer version of the same diameter and number of turns, the
bunched
baluns show a large downward shift in parallel self-resonance frequency and
poor choking reactance at the higher frequencies.
Interpreting the Measurements
-----------------------------
All the baluns start out looking inductive at low frequencies, as indicated
by
the positive phase angles. As the frequency is increased, a point is
reached
where the capacitance between the windings forms a parallel resonance with
the
coil's inductance. Above this frequency, the winding reactance is reduced
by
this capacitance. The interwinding capacitance increases with the number of
turns and the diameter of the turns, so "more is not always better".
The effects of a large increase in interwinding capacitance is evident in
the
measurements on the balun with the bunched turns. This is probably a result
of the first and last turns of the coil being much closer together than the
single-layer coil.
An important requirement of these baluns is that the magnitude of the
winding
reactance be much greater than the load impedance. In the case of a 50 ohm
balanced antenna, the balun's winding impedance is effectively shunted
across
one half the 50 ohm load impedance, or 25 ohms. A reasonable critera for
the
balun's winding impedance for negligible common mode current in the shield
is
that it be at least 20 times this, or 500 ohms. The measurements show, for
example, that 6 turns 4-1/4 inches in diameter meet this criteria from 14 to
35 MHz.
The measurement data also reveals the power loss these baluns will exhibit.
Each of the measurement points can be transformed from the polar format of
the
table to a parallel equivalent real and reactive shunt impedance. The power
dissipated in the balun is then the square of the voltage across it divided
by
the real parallel equivalent shunt impedance. While this calculation can be
made for each measurement point, an approximate number can be taken directly
from the tables at the parallel resonance points. At 0 degrees phase angle
the magnitude numbers are pure resistive. I didn't record the exact
resonance
points, but it can be seen from the tables that the four single-layer baluns
are all above 15K ohms, while the ferrite bead balun read about 1.4K. These
baluns see half the load voltage, so at 1500 watts to a 50 ohm load, the
power
dissipated in the coaxial baluns will be less than 1.3 watts, and the
ferrite
bead balun will dissipate about 13.4 watts (neglecting possible core
saturation and other non-linear effects). These losses are certainly
negligible. At 200 ohms load impedance, the losses are under 5 watts for
the
coaxial baluns and 53.6 watts for the ferrite beads.
Conclusions
-----------
- A 1:1 coaxial balun with excellent choking reactance for 10 through 20
meters can be made by winding 6 turns of RG-213 on inexpensive 4 inch PVC
sewer pipe.
- For 40 or 30 meters, use 12 turns of RG-213 on 4 inch PVC sewer pipe.
- Don't bunch the turns together. Wind them as a single layer on a form.
Bunching the turns kills the choking effect at higher
frequencies.
- Don't use too many turns. For example, the HyGain manuals for my 10 and
15
meter yagis both recommend 12 turns 6 inches in diameter. At the very least
this is about 3 times as much coax as is needed, and these dimensions
actually
give less than the desired choking impedance on 10 and 15 meters.
Measurements
------------
Magnitude in ohms, phase angle in degrees, as a function of frequency in Hz,
for various baluns.
6 Turns 12 Turns 4 Turns 8 Turns 8 Turns
Ferrite
4-1/4 in 4-1/4 in 6-5/8 in 6-5/8 in 6-5/8 in
beads
sngl layer sngl layer sngl layer sngl layer bunched
(Aztec)
---------- ---------- ---------- ---------- ----------
----------
Frequency Mag Phase Mag Phase Mag Phase Mag Phase Mag Phase Mag
Phase
1.00E+06 26 88.1 65 89.2 26 88.3 74 89.2 94 89.3 416
78.1
2.00E+06 51 88.7 131 89.3 52 88.8 150 89.3 202 89.2 795
56.1
3.00E+06 77 88.9 200 89.4 79 89.1 232 89.3 355 88.9 1046
39.8
4.00E+06 103 89.1 273 89.5 106 89.3 324 89.4 620 88.3 1217
26.6
5.00E+06 131 89.1 356 89.4 136 89.2 436 89.3 1300 86.2 1334
14.7
6.00E+06 160 89.3 451 89.5 167 89.3 576 89.1 8530 59.9 1387
3.6
7.00E+06 190 89.4 561 89.5 201 89.4 759 89.1 2120 -81.9 1404
-5.9
8.00E+06 222 89.4 696 89.6 239 89.4 1033 88.8 1019 -85.7 1369
-15.4
9.00E+06 258 89.4 869 89.5 283 89.4 1514 87.3 681 -86.5 1295
-23.7
1.00E+07 298 89.3 1103 89.3 333 89.2 2300 83.1 518 -86.9 1210
-29.8
1.10E+07 340 89.3 1440 89.1 393 89.2 4700 73.1 418 -87.1 1123
-35.2
1.20E+07 390 89.3 1983 88.7 467 88.9 15840 -5.2 350 -87.2 1043
-39.9
1.30E+07 447 89.2 3010 87.7 556 88.3 4470 -62.6 300 -86.9 954
-42.7
1.40E+07 514 89.3 5850 85.6 675 88.3 2830 -71.6 262 -86.9 901
-45.2
1.50E+07 594 88.9 42000 44.0 834 87.5 1910 -79.9 231 -87.0 847
-48.1
1.60E+07 694 88.8 7210 -81.5 1098 86.9 1375 -84.1 203 -87.2 778
-51.8
1.70E+07 830 88.1 3250 -82.0 1651 81.8 991 -82.4 180 -86.9 684
-54.4
1.80E+07 955 86.0 2720 -76.1 1796 70.3 986 -67.2 164 -84.9 623
-45.9
1.90E+07 1203 85.4 1860 -80.1 3260 44.6 742 -71.0 145 -85.1 568
-51.2
2.00E+07 1419 85.2 1738 -83.8 3710 59.0 1123 -67.7 138 -84.5 654
-34.0
2.10E+07 1955 85.7 1368 -87.2 12940 -31.3 859 -84.3 122 -86.1 696
-49.9
2.20E+07 3010 83.9 1133 -87.8 3620 -77.5 708 -86.1 107 -85.9 631
-54.8
2.30E+07 6380 76.8 955 -88.0 2050 -83.0 613 -86.9 94 -85.5 584
-57.4
2.40E+07 15980 -29.6 807 -86.3 1440 -84.6 535 -86.3 82 -85.0 536
-58.8
2.50E+07 5230 -56.7 754 -82.2 1099 -84.1 466 -84.1 70 -84.3 485
-59.2
2.60E+07 3210 -78.9 682 -86.4 967 -83.4 467 -81.6 60 -82.7 481
-56.2
2.70E+07 2000 -84.4 578 -87.3 809 -86.5 419 -85.5 49 -81.7 463
-60.5
2.80E+07 1426 -85.6 483 -86.5 685 -87.1 364 -86.2 38 -79.6 425
-62.5
2.90E+07 1074 -85.1 383 -84.1 590 -87.3 308 -85.6 28 -75.2 387
-63.8
3.00E+07 840 -83.2 287 -75.0 508 -87.0 244 -82.1 18 -66.3 346
-64.4
3.10E+07 661 -81.7 188 -52.3 442 -85.7 174 -69.9 9 -34.3 305
-64.3
3.20E+07 484 -78.2 258 20.4 385 -83.6 155 -18.0 11 37.2 263
-63.2
3.30E+07 335 -41.4 1162 -13.5 326 -78.2 569 -0.3 21 63.6 212
-58.0
3.40E+07 607 -32.2 839 -45.9 316 -63.4 716 -57.6 32 71.4 183
-40.5
3.50E+07 705 -58.2 564 -56.3 379 -69.5 513 -72.5 46 76.0 235
-29.6
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