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-   -   160 meter mobile -- Reality Check (https://www.radiobanter.com/antenna/67151-160-meter-mobile-reality-check.html)

RST Engineering March 19th 05 08:45 PM

160 meter mobile -- Reality Check
 
My bag is VHF, so forgive me if I've bumbled up the calculations. My
numbers show that a standard 108" whip has an input impedance of somewhere
around 0.04 ohms in series with a 22 pf capacitor.

These numbers are so far from what I normally deal with that I'm not sure
that I'm right, and I'd appreciate somebody who actually works down in this
area giving my numbers a reality check.

If they ARE right, how in heaven do most people match to 0.04 ohms? The 22
pf I can resonate out with a 1 millihenry choke (or thereabouts), but how do
most people match 50 ohms to fractional ohms in the homebrew arena -- that
is, without just going out and buying a "magical matching box" of some sort?

Jim



Wes Stewart March 19th 05 10:28 PM

On Sat, 19 Mar 2005 12:45:53 -0800, "RST Engineering"
wrote:

My bag is VHF, so forgive me if I've bumbled up the calculations. My
numbers show that a standard 108" whip has an input impedance of somewhere
around 0.04 ohms in series with a 22 pf capacitor.


Not quite. Over perfect ground the Z is ~ 0.37 -j8170 @ 1.9 MHz for a
12mm diameter radiator.

So you add an inductor of +j8170 with say Q=250. That gives Z =
(0.37+32.68) +j0 = 33.05 +j0. Then you add 16.95 ohm of ground loss
and Z = 50 +j0.

A perfect match with a gain of -17 dBi. :) Easy huh?


These numbers are so far from what I normally deal with that I'm not sure
that I'm right, and I'd appreciate somebody who actually works down in this
area giving my numbers a reality check.

If they ARE right, how in heaven do most people match to 0.04 ohms? The 22
pf I can resonate out with a 1 millihenry choke (or thereabouts), but how do
most people match 50 ohms to fractional ohms in the homebrew arena -- that
is, without just going out and buying a "magical matching box" of some sort?

Jim



[email protected] March 19th 05 10:30 PM

RST Engineering wrote:
My bag is VHF, so forgive me if I've bumbled up the calculations. My


numbers show that a standard 108" whip has an input impedance of

somewhere
around 0.04 ohms in series with a 22 pf capacitor.

These numbers are so far from what I normally deal with that I'm not

sure
that I'm right, and I'd appreciate somebody who actually works down

in this
area giving my numbers a reality check.

If they ARE right, how in heaven do most people match to 0.04 ohms?

The 22
pf I can resonate out with a 1 millihenry choke (or thereabouts), but

how do
most people match 50 ohms to fractional ohms in the homebrew arena --

that
is, without just going out and buying a "magical matching box" of

some sort?

Jim

Hi Jim, Your numbers look about right for a 108" whip on 1.8mhz. To
feed a small whip like this you would have to "brute force" it with a
large loading coil at the base. The efficiency will be low and the
bandwidth narrow. To get any efficiency at all, the 2:1 swr bandwidth
will only be around 5khz. Once you tune it up, it will be a single
frequency antenna.
There are things like adding capacitive loading at the top of the
whip, and moving the inductive loading to the center (have to cut the
whip in half). This will make the feedpoint Z a little more managable.
I once loaded an 8' antenna on 160, just to see if I could, but never
got on the air with it. I read somewhere that in the 50's, law
enforcement 2-way radios operated close to our 160m ham band. Wonder
what kind of antennas they used on the police cars. Of course the
distances they were interested in are different from hams.
Gary N4AST


Frank March 19th 05 11:23 PM


"Wes Stewart" wrote in message
...
On Sat, 19 Mar 2005 12:45:53 -0800, "RST Engineering"
wrote:

My bag is VHF, so forgive me if I've bumbled up the calculations. My
numbers show that a standard 108" whip has an input impedance of somewhere
around 0.04 ohms in series with a 22 pf capacitor.


Not quite. Over perfect ground the Z is ~ 0.37 -j8170 @ 1.9 MHz for a
12mm diameter radiator.

So you add an inductor of +j8170 with say Q=250. That gives Z =
(0.37+32.68) +j0 = 33.05 +j0. Then you add 16.95 ohm of ground loss
and Z = 50 +j0.

A perfect match with a gain of -17 dBi. :) Easy huh?


These numbers are so far from what I normally deal with that I'm not sure
that I'm right, and I'd appreciate somebody who actually works down in
this
area giving my numbers a reality check.

If they ARE right, how in heaven do most people match to 0.04 ohms? The
22
pf I can resonate out with a 1 millihenry choke (or thereabouts), but how
do
most people match 50 ohms to fractional ohms in the homebrew arena -- that
is, without just going out and buying a "magical matching box" of some
sort?

Jim



The following code produces Zin = 0.117 - j2717 ohms at 1.9 MHz. What did
I do wrong? Note the high segmentation to place the feed-point near the
base of the antenna.

Frank

CM 9 ft monopole
CE
GW 1 108 0 0 0 0 0 108 0.25
GS 0 0 0.025400
GE 1
GN 1
EX 0 1 1 00 1 0
LD 5 1 1 108 5.8001E7
FR 0 9 0 0 1.8 0.025
RP 0 181 1 1000 -90 0 1.00000 1.00000
EN



Roy Lewallen March 20th 05 12:02 AM

Frank wrote:

The following code produces Zin = 0.117 - j2717 ohms at 1.9 MHz. What did
I do wrong? Note the high segmentation to place the feed-point near the
base of the antenna.

Frank

CM 9 ft monopole
CE
GW 1 108 0 0 0 0 0 108 0.25
GS 0 0 0.025400
GE 1
GN 1
EX 0 1 1 00 1 0
LD 5 1 1 108 5.8001E7
FR 0 9 0 0 1.8 0.025
RP 0 181 1 1000 -90 0 1.00000 1.00000
EN


If you follow NEC guidelines on the minimum recommended segment
length/wire radius ratio, you should have no more than 17 segments; the
model has 127. In this case, though, it doesn't seem to be disturbing
NEC-2 very much. Also, the half inch diameter is somewhat greater than
most CB whips. If you drop the diameter to a quarter inch, you'll get a
substantially greater reactance which would require a larger loading
inductor and hence result in lower efficiency. Otherwise it looks ok to me.

As Wes pointed out, the ground system and loading inductor losses will
be so large as to make the feedpoint resistance (and wire loss)
insignificant. The zero-loss feedpoint resistance is, however, useful in
determining efficiency. If you set the wire loss to zero by removing the
LD "card", you get the more useful value of feedpoint resistance when
losses are zero, 0.098 ohms. Using Wes' value of about 50 ohm feedpoint
resistance when losses are included, you can calculate the efficiency as
0.098/50 = 0.2%, or 2 watts radiated for each kW applied. In American
mobile terms that's 1.5 watts per horsepower. I'm always glad to see
more QRP signals on the band.

Roy Lewallen, W7EL

Reg Edwards March 20th 05 12:05 AM

To obtain obtain some idea of the numerical values involved with
mobile, short, antennas on 160 meter and other low frequency bands,
download programs -

HELICAL3
VERTLOAD
LOADCOIL

from website below. Takes only a few seconds to download. Not zipped
up. Run immediately.

With a very short antenna, to obtain a useful efficiency, a physically
large loading coil is essential. The only space available is up the
antenna. So the best thing to do is extend the coil up the antenna
from near the base, in the form of a long slender helical winding on a
pvc plastic pipe.

The whole thing behaves as a short 1/4-wave resonant vertical. There
is a short rod at the top which is pruned to resonate the antenna in
the required band. It is inevitably a single frequency job. The
bandwidth on 160m is only a few kHz.

With a 100 watt transmitter, when both vehicles are in the low-noise
countryside, it is possible to work 100 miles or more, on groundwave,
in daylight. Much further via skywave in darkness. G3YXM has worked
transatlantic from a car in Scotland to a base station in Canada on
occasions.

Maximum overall antenna heights are about 9 feet above roof of car
with the coil about 2" in diameter, the coil extending to a height of
6 or 7 feet.

The most tedious procedure is pruning all antenas in a group of
mobiles to the same frequency on the 160 meter band. But it has been
done. Mobile to a base station is easy. For many years the standard
UK frequency for mobiles was 1930 kHz.

Matching from antenna base to a 50-ohm transmiier can be accomplished
by a single or bank of mica capacitors of several hundred pF.

For quite a number of years, mobile working on 160m was quite popular
in the UK using helically-wound antennas.
----
.................................................. ..........
Regards from Reg, G4FGQ
For Free Radio Design Software go to
http://www.btinternet.com/~g4fgq.regp
.................................................. ..........



[email protected] March 20th 05 12:18 AM


Frank wrote:
"Wes Stewart" wrote in message
...
On Sat, 19 Mar 2005 12:45:53 -0800, "RST Engineering"
wrote:

My bag is VHF, so forgive me if I've bumbled up the calculations.

My
numbers show that a standard 108" whip has an input impedance of

somewhere
around 0.04 ohms in series with a 22 pf capacitor.


Not quite. Over perfect ground the Z is ~ 0.37 -j8170 @ 1.9 MHz

for a
12mm diameter radiator.

So you add an inductor of +j8170 with say Q=250. That gives Z =
(0.37+32.68) +j0 = 33.05 +j0. Then you add 16.95 ohm of ground

loss
and Z = 50 +j0.

A perfect match with a gain of -17 dBi. :) Easy huh?


These numbers are so far from what I normally deal with that I'm

not sure
that I'm right, and I'd appreciate somebody who actually works down

in
this
area giving my numbers a reality check.

If they ARE right, how in heaven do most people match to 0.04 ohms?

The
22
pf I can resonate out with a 1 millihenry choke (or thereabouts),

but how
do
most people match 50 ohms to fractional ohms in the homebrew arena

-- that
is, without just going out and buying a "magical matching box" of

some
sort?

Jim



The following code produces Zin = 0.117 - j2717 ohms at 1.9 MHz.

What did
I do wrong? Note the high segmentation to place the feed-point near

the
base of the antenna.

Frank

CM 9 ft monopole
CE
GW 1 108 0 0 0 0 0 108 0.25
GS 0 0 0.025400
GE 1
GN 1
EX 0 1 1 00 1 0
LD 5 1 1 108 5.8001E7
FR 0 9 0 0 1.8 0.025
RP 0 181 1 1000 -90 0 1.00000 1.00000
EN


Hi Frank, Well, I got different numbers than both of you. Must depend
on the ground type of the models, as well as the # of segments.
If you are trying to match an antenna with fractions of an ohm
resistive and thousands reactive, the differences we are all observing
will not make a whole lot of difference in the matching network you
decide to use. It will be big and bulky, and very inefficient.
Gary N4AST


Wes Stewart March 20th 05 12:52 AM

On Sat, 19 Mar 2005 23:23:30 GMT, "Frank"
wrote:

[snip]

The following code produces Zin = 0.117 - j2717 ohms at 1.9 MHz. What did
I do wrong? Note the high segmentation to place the feed-point near the
base of the antenna.

Frank

CM 9 ft monopole
CE
GW 1 108 0 0 0 0 0 108 0.25
GS 0 0 0.025400
GE 1
GN 1
EX 0 1 1 00 1 0
LD 5 1 1 108 5.8001E7
FR 0 9 0 0 1.8 0.025
RP 0 181 1 1000 -90 0 1.00000 1.00000
EN


My bad. I hate it when that happens. A typo on the length on my
part. 101 instead of 108.

It's more like 0.12 -j2890 in EZNEC. I'm not real fluent in NEC decks
but I think you are using too many segments.




Frank March 20th 05 01:42 AM


"Roy Lewallen" wrote in message
...
Frank wrote:

The following code produces Zin = 0.117 - j2717 ohms at 1.9 MHz. What
did I do wrong? Note the high segmentation to place the feed-point near
the base of the antenna.

Frank

CM 9 ft monopole
CE
GW 1 108 0 0 0 0 0 108 0.25
GS 0 0 0.025400
GE 1
GN 1
EX 0 1 1 00 1 0
LD 5 1 1 108 5.8001E7
FR 0 9 0 0 1.8 0.025
RP 0 181 1 1000 -90 0 1.00000 1.00000
EN


If you follow NEC guidelines on the minimum recommended segment
length/wire radius ratio, you should have no more than 17 segments; the
model has 127. In this case, though, it doesn't seem to be disturbing
NEC-2 very much. Also, the half inch diameter is somewhat greater than
most CB whips. If you drop the diameter to a quarter inch, you'll get a
substantially greater reactance which would require a larger loading
inductor and hence result in lower efficiency. Otherwise it looks ok to
me.

As Wes pointed out, the ground system and loading inductor losses will be
so large as to make the feedpoint resistance (and wire loss)
insignificant. The zero-loss feedpoint resistance is, however, useful in
determining efficiency. If you set the wire loss to zero by removing the
LD "card", you get the more useful value of feedpoint resistance when
losses are zero, 0.098 ohms. Using Wes' value of about 50 ohm feedpoint
resistance when losses are included, you can calculate the efficiency as
0.098/50 = 0.2%, or 2 watts radiated for each kW applied. In American
mobile terms that's 1.5 watts per horsepower. I'm always glad to see more
QRP signals on the band.

Roy Lewallen, W7EL


I should have read the manual before modeling, but I was so concerned that
the feed-point be near the bottom. Changing the segmentation to 17,
removing the LD card, and reducing the radius to 0.125 ", calculates the
feed-point impedance as: 0.123 - j3286. I considered Jim's calculation of
0.37 - j8170 to be far too reactive. The fact is these points are so close,
when observed on the Smith chart, as to be virtually identical.

Analyzing a shunt L/series C matching network, with inductor Q at 300,
indicates a loss of 21.5dB with 30 kV RMS at the base of the antenna (1.5 kW
into the matching network). (In the case of 0.37 - j8170 the loss is 21.8
dB, with 42 kV at the base). These voltages are so large, I am beginning to
wonder if I goofed again! The losses, at least, are the same order of
magnitude as Roy's calculation.

73,

Frank



Roy Lewallen March 20th 05 02:41 AM

If you had made this model with EZNEC, you would have seen a warning
that the segment length is shorter than recommended. And you could have
entered the dimensions directly in inches (or immediately converted
between meters and inches). The free demo program is adequate for this
model, providing you don't want more than 20 segments.

Roy Lewallen, W7EL

Frank wrote:

I should have read the manual before modeling, but I was so concerned that
the feed-point be near the bottom. Changing the segmentation to 17,
removing the LD card, and reducing the radius to 0.125 ", calculates the
feed-point impedance as: 0.123 - j3286. I considered Jim's calculation of
0.37 - j8170 to be far too reactive. The fact is these points are so close,
when observed on the Smith chart, as to be virtually identical.

Analyzing a shunt L/series C matching network, with inductor Q at 300,
indicates a loss of 21.5dB with 30 kV RMS at the base of the antenna (1.5 kW
into the matching network). (In the case of 0.37 - j8170 the loss is 21.8
dB, with 42 kV at the base). These voltages are so large, I am beginning to
wonder if I goofed again! The losses, at least, are the same order of
magnitude as Roy's calculation.

73,

Frank



Frank March 20th 05 06:21 PM

"Wes Stewart" wrote in message
...
On Sat, 19 Mar 2005 23:23:30 GMT, "Frank"
wrote:

[snip]

The following code produces Zin = 0.117 - j2717 ohms at 1.9 MHz. What did
I do wrong? Note the high segmentation to place the feed-point near the
base of the antenna.

Frank

CM 9 ft monopole
CE
GW 1 108 0 0 0 0 0 108 0.25
GS 0 0 0.025400
GE 1
GN 1
EX 0 1 1 00 1 0
LD 5 1 1 108 5.8001E7
FR 0 9 0 0 1.8 0.025
RP 0 181 1 1000 -90 0 1.00000 1.00000
EN


My bad. I hate it when that happens. A typo on the length on my
part. 101 instead of 108.

It's more like 0.12 -j2890 in EZNEC. I'm not real fluent in NEC decks
but I think you are using too many segments.


A more realistic analysis than above, with the following structure, produces
some interesting results:
9ft monopole, segmented in 12" lengths, mounted above a 6' x 6' wire grid
model, also 12" segments, (All wires # 10 AWG). 5 ft above a
Sommerfeld/Norton average ground (Er = 13, Sigma = 5 mS/m). Frequency 1.9
MHz.

Zin = 1.23 - j3059, max gain = -8.3 dBi at 25 deg. elevation. (surface
wave not computed). Structure
efficiency 98.7%.

A suitable matching network, assuming an inductor Q of 300, consists of a
shunt "L" (161uH) followed by a
series C (16.2 pF). The network loss is 11.5 dB and 28 kV RMS at the base
with 1.5 kW in.

With an inductor Q of 1000, the component values become: L = 193.5 uH, and C
= 8.88 pF.
Loss = 6.3 dB, and 51 kV RMS.

Frank

Edited code follows:

CM 9 ft monopole above 6ft X 6ft wire grid gp
CE
GW 1 9 0 0 14 0 0 5 0.0509449
GW 2 1 -3 -3 5 -2 -3 5 0.0509449
|
|
GW 85 1 3 2 5 3 3 5 0.0509449
GS 0 0 0.304800
GE 1
GN 2 0 0 0 13.0000 0.0050
EX 0 1 9 0 1 0
LD 5 1 1 9 5.8001E7
LD 5 2 1 1 5.8001E7
|
|
LD 5 85 1 1 5.8001E7
FR 0 9 0 0 1.8 0.025
RP 0 181 1 1000 -90 0 1 1
EN



Crazy George March 25th 05 04:35 AM

Gary:

First, you are off by a decade, the Texas DPS moved from 1658 kcps. to 42.9 Mc. in 1949. Prior to the move, they used
(very successfully, I might add) a earlier version of Reg's antenna, which was a 10 foot bamboo pole helically wound
with waxed cotton insulated bell wire. IIRC, the winding was spaced about 1 to 1½ wire diameters apart . The
transmitter was directly connected to the base of the antenna with a short piece of 8 gauge wire, so there was no SWR to
worry about, and final tuning of the antenna was done in the transmitter output pi-network. Black '41 and '48 Fords
with 10 foot cane poles on the rear bumper brackets, brings back memories.

--
Crazy George
The attglobal.net address is a SPAM trap. Please change that part to: attdotbiz properly formatted.
wrote in message ups.com...

snippety

I read somewhere that in the 50's, law
enforcement 2-way radios operated close to our 160m ham band. Wonder
what kind of antennas they used on the police cars. Of course the
distances they were interested in are different from hams.
Gary N4AST




[email protected] March 26th 05 12:35 AM


Crazy George wrote:
Gary:

First, you are off by a decade, the Texas DPS moved from 1658 kcps.

to 42.9 Mc. in 1949. Prior to the move, they used
(very successfully, I might add) a earlier version of Reg's antenna,

which was a 10 foot bamboo pole helically wound
with waxed cotton insulated bell wire. IIRC, the winding was spaced

about 1 to 1=BD wire diameters apart . The
transmitter was directly connected to the base of the antenna with a

short piece of 8 gauge wire, so there was no SWR to
worry about, and final tuning of the antenna was done in the

transmitter output pi-network. Black '41 and '48 Fords
with 10 foot cane poles on the rear bumper brackets, brings back

memories.

--
Crazy George
The attglobal.net address is a SPAM trap. Please change that part

to: attdotbiz properly formatted.
wrote in message

ups.com...

snippety

I read somewhere that in the 50's, law
enforcement 2-way radios operated close to our 160m ham band.

Wonder
what kind of antennas they used on the police cars. Of course the
distances they were interested in are different from hams.
Gary N4AST


Hi C. George, Thanks for the interesting info. I certainly did not
know the 160m radios dated to the 40's. My memories of 1950's law
enforcement are "Highway Patrol" starring Broderick Crawford on the BW
TV. I remember watching him standing outside his police car and saying
"10-4" into the mike. Then, he would sometimes put the mike to his
ear, as if it were a speaker.
At the time I didn't wonder about the antenna on his car. I would
expect from your post it would be 43mhz. I don't remember if that show
was any good or not?
Gary N4AST


J. Mc Laughlin March 26th 05 02:37 AM

Chicago once dispatched their cars on a frequency of about 1700 kHz. Used
to listen with a Wilcox-Gay receiver (made in Charlotte, Michigan) that had
a knob used to switch from broadcast band to the MF police band. Long time
ago!
I was of the opinion that the Chicago system was one way. Does anyone
remember?
Some of the police HF frequencies were used on CW into at least the
mid-60s. They were not allowed to use RTTY as it was thought to compete too
much with The telephone company. I visited the main HF site for Ohio in the
early 60s - the site was controlled from Columbus with a microwave link.
The engineer liked to call it the longest IF in the world.

73, Mac N8TT

--
J. Mc Laughlin; Michigan U.S.A.
Home:



Butch March 26th 05 08:05 AM

My dad was a policeman in the 40s, right after the war, his operated 40
something mHz. About 8 yrs old and an interest in radio helped me to
remember radio things, many other things didn't have sticking power,
like english and such :o)

KF5DE

wrote:
Crazy George wrote:

Gary:

First, you are off by a decade, the Texas DPS moved from 1658 kcps.


to 42.9 Mc. in 1949. Prior to the move, they used

(very successfully, I might add) a earlier version of Reg's antenna,


which was a 10 foot bamboo pole helically wound

with waxed cotton insulated bell wire. IIRC, the winding was spaced


about 1 to 1½ wire diameters apart . The

transmitter was directly connected to the base of the antenna with a


short piece of 8 gauge wire, so there was no SWR to

worry about, and final tuning of the antenna was done in the


transmitter output pi-network. Black '41 and '48 Fords

with 10 foot cane poles on the rear bumper brackets, brings back


memories.

--
Crazy George
The attglobal.net address is a SPAM trap. Please change that part


to: attdotbiz properly formatted.

wrote in message


ups.com...

snippety

I read somewhere that in the 50's, law
enforcement 2-way radios operated close to our 160m ham band.


Wonder

what kind of antennas they used on the police cars. Of course the
distances they were interested in are different from hams.
Gary N4AST



Hi C. George, Thanks for the interesting info. I certainly did not
know the 160m radios dated to the 40's. My memories of 1950's law
enforcement are "Highway Patrol" starring Broderick Crawford on the BW
TV. I remember watching him standing outside his police car and saying
"10-4" into the mike. Then, he would sometimes put the mike to his
ear, as if it were a speaker.
At the time I didn't wonder about the antenna on his car. I would
expect from your post it would be 43mhz. I don't remember if that show
was any good or not?
Gary N4AST



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