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[email protected] April 5th 05 04:59 AM


"Richard Harrison" wrote in message
...
Art, KB9MZ wrote:
"O.K. Reg, I`ll take you up on the 50 dB F/B."

It requires good balance for such cancellation.


Yes, it will not come by accident but Reg has said that 50 db F/B is
"silly"!
Why would he say that without back up evidence? He also did not offer
a max F/B that was obtainable in theory. I have seen computor results
that offer 50 db F/B based on NEC, Can I trust gain if F/B cannot
be trusted? Obviously 50 db is hard to get but is it beyond the realms
of possibility?
The F/B that you offered is a bit unfair but then it is an antenna and
Reg did not qualify his statement.
I personaly modelled a antenna that comprised of a driven element
with the remaining elements acting as reflectors only. And we all know
that extra reflectors are a waste of time for H.F.( grin ) but they do give
very high F/B figures.
I wonder what a corner reflector antenna would provide

Regards
Art KB9MZ......XG


Kraus gives the gain for a 100-meter dish near Bonn, Germany on page 676
of the 3rd edition of "Antennas". Gain is a function of frequency and
varies from about 48 dB at 300 MHz to about 98 dB at 150 GHz. I don`t
know if shielding has been added to make this a "high-performance" dish
but I would wager that this enormous radio ear and mouth has an
excellent front-to-back ratio. Probably exceeds forward gain at some
azimuths and elevation angles.

Arnold B. Bailey has a lot to say anout a "connected" (driven) element
and a parasitic reflector, starting about on 447 of "TV and Other
Receiving Antennas", Bailey says:
"The optimum spacing for highest gain of a parasitic reflector is S=0.15
wavelength plus or minus 0.025. Here the relleector is operated at Q=+1
(longer than resonant) and the gain in direction 1 is approximately 5.5
dB. Reasonable compromise for a less critical system is to use a spacing
of 0.2 wavelength and a parasitic element longer than resonant (at
Q=+1). This case gives a gain in direction 1 of 5 dB."

On page 440 Bailey says: The front-to-back ratio ---is 17.5 dB in this
case, and the Y/X ratio only about 9 dB, where +X represents the optimum
direction.---" A picture is worth 1000 words.

Best regards, Richard Harrison, KB5WZI




John Smith April 5th 05 05:38 AM

Just for the sake of curriosity: what if a RASER "Radio (frequency)
Amplification by Stimulated Emission of Radiation" device existed?
50 db would become acceptable and common place overnight, huh? MASER's
exist, why now long wavelength? Sure the antenna at HF would be the size of
the pentagon, but Bill Gates wouldn't blink an eye! grin

Regards

--
I would like to point out, I do appreciate the "Been there--done that!"
posts. Indeed, now your observations, comments and discourse should be
filled with wisdom--I am listening!!!
" wrote in message
news:P2o4e.22497$NW5.1099@attbi_s02...

"Richard Harrison" wrote in message
...
Art, KB9MZ wrote:
"O.K. Reg, I`ll take you up on the 50 dB F/B."

It requires good balance for such cancellation.


Yes, it will not come by accident but Reg has said that 50 db F/B is
"silly"!
Why would he say that without back up evidence? He also did not offer
a max F/B that was obtainable in theory. I have seen computor results
that offer 50 db F/B based on NEC, Can I trust gain if F/B cannot
be trusted? Obviously 50 db is hard to get but is it beyond the realms
of possibility?
The F/B that you offered is a bit unfair but then it is an antenna and
Reg did not qualify his statement.
I personaly modelled a antenna that comprised of a driven element
with the remaining elements acting as reflectors only. And we all know
that extra reflectors are a waste of time for H.F.( grin ) but they do
give
very high F/B figures.
I wonder what a corner reflector antenna would provide

Regards
Art KB9MZ......XG


Kraus gives the gain for a 100-meter dish near Bonn, Germany on page 676
of the 3rd edition of "Antennas". Gain is a function of frequency and
varies from about 48 dB at 300 MHz to about 98 dB at 150 GHz. I don`t
know if shielding has been added to make this a "high-performance" dish
but I would wager that this enormous radio ear and mouth has an
excellent front-to-back ratio. Probably exceeds forward gain at some
azimuths and elevation angles.

Arnold B. Bailey has a lot to say anout a "connected" (driven) element
and a parasitic reflector, starting about on 447 of "TV and Other
Receiving Antennas", Bailey says:
"The optimum spacing for highest gain of a parasitic reflector is S=0.15
wavelength plus or minus 0.025. Here the relleector is operated at Q=+1
(longer than resonant) and the gain in direction 1 is approximately 5.5
dB. Reasonable compromise for a less critical system is to use a spacing
of 0.2 wavelength and a parasitic element longer than resonant (at
Q=+1). This case gives a gain in direction 1 of 5 dB."

On page 440 Bailey says: The front-to-back ratio ---is 17.5 dB in this
case, and the Y/X ratio only about 9 dB, where +X represents the optimum
direction.---" A picture is worth 1000 words.

Best regards, Richard Harrison, KB5WZI






Jerry Martes April 5th 05 06:59 AM


Roy

When I was working with antennas, we considered the antenna's F/B ratio
used the max of the front compared to the max of the back. But, I get the
impression that the rules are different now.

Jerry


"Roy Lewallen" wrote in message
...
wrote:
. . .
I have seen computor results
that offer 50 db F/B based on NEC, Can I trust gain if F/B cannot
be trusted?


Absolutely! While you might get some very deep nulls at some particular
points in space, and fairly deep nulls in some particular
azimuth/elevation angle combinations, they're not likely to be exactly as
deep or in the directions the program reports. Gain, on the other hand,
can be strikingly accurate in many cases.

Put together any model you want with an extreme F/B ratio. Then fiddle the
model just slightly -- change the frequency, element length or diameter,
etc. Look at how much the gain changes, and how much the F/B changes.
Modify it more, and look again.

You'll see that the F/B is *much* more critical than gain. You can goof up
the model -- or real antenna -- a lot more without any appreciable change
in gain than you can before seeing major changes in F/B.

The reason is simple. To get a deep null and therefore good F/B ratio, you
have to add the fields from all parts of the antenna together to get zero
within a tiny, tiny fraction of a percent. If any one of the fields
changes just a tiny amount, they no longer sum precisely to zero. But
small change like that won't noticeably affect the gain. No model is good
enough to precisely predict extremely deep nulls -- there's always too
much difference between the model and reality.

I don't recall what Reg recently said, but I've gotten 50 dB and greater
F/B ratios from an array by adjusting the phasing network while listening
to a receiver placed in the null direction. But the null is that deep only
in that direction, at that height above ground. It's also noticeably
shallower a little ways away even in the same direction, because I've
compensated for re-radiation from nearby objects, too. Even coax shield
leakage becomes a very noticeable factor. So while I can tweak an array to
get a very deep null, there's no way I can expect that to hold when
anything changes, even just a little. I'd even expect it to change from
day to day as the ground moisture changes and the sap rises in the trees.

Obviously 50 db is hard to get but is it beyond the realms
of possibility?


For what, one particular azimuth/elevation combination at one single
frequency? You might be able to do it. But it would be only of academic
interest at best.

. . .


Roy Lewallen, W7EL




Roy Lewallen April 5th 05 07:21 AM

What are "front" and "back"? If the maximum forward lobe is +10 dBi at
an elevation angle of 23 degrees and the best null is -30 dBi at an
azimuth angle 160 degrees from the peak forward lobe, and at an
elevation angle of 47 degrees, are you saying that by your definition
the front/back ratio is 40 dB? If so, I guess that's interesting but I
can't imagine what it might be good for.

Who's "we"?

Roy Lewallen, W7EL

Jerry Martes wrote:
Roy

When I was working with antennas, we considered the antenna's F/B ratio
used the max of the front compared to the max of the back. But, I get the
impression that the rules are different now.

Jerry


Jerry Martes April 5th 05 09:14 AM

Roy

I make no claim to being qualified to discuss antennas with you when we
are in disagreement. I worked as an antenna design engineer for 15 years
till 1968 when I was layed off from TRW. I was never a high level theorist
but managed to hold a decent position with designing hardware. I did work
with some highly qualified engineers from whom I thought I obtained alot of
knowledge about antennas. Thats why I was bold enough to say "we". I
still maintain a casual relationship with George Oltman who you might know
from his association with antenna groups with IEEE.
As for the F/B, I considered that to identify Front to Back of the
antenna's radiation pattern. I would consider it appropriate to identify
the radiation toward the "Front" as the max radiation to the front. Then,
it seems that the numerical level used for the "F/B ratio" should be max to
the Back.
I make no argument that this definition I use is *the* way F/B is. But,
dont we define "side lobe level" as the ratio of the main beam Max to the
side lobe Max? Be aware, I dont write to correct your thinking. I did
consider the F/B to be flawed when the main beam Max is compared with a rear
radiation Min.

I'll consider myself corrected and stop posting.

Jerry

"Roy Lewallen" wrote in message
...
What are "front" and "back"? If the maximum forward lobe is +10 dBi at an
elevation angle of 23 degrees and the best null is -30 dBi at an azimuth
angle 160 degrees from the peak forward lobe, and at an elevation angle of
47 degrees, are you saying that by your definition the front/back ratio is
40 dB? If so, I guess that's interesting but I can't imagine what it might
be good for.

Who's "we"?

Roy Lewallen, W7EL

Jerry Martes wrote:
Roy

When I was working with antennas, we considered the antenna's F/B ratio
used the max of the front compared to the max of the back. But, I get
the impression that the rules are different now.

Jerry




[email protected] April 5th 05 02:03 PM

Don't quit posting Jerry, you are an asset to the group.
It is just that courtesy is not a requirement in this group
so some posts tend to be a bit sharp and personal
Look forward to hearing from you again
Regards
Art






"Jerry Martes" wrote in message
news:xNr4e.3912$%b1.1814@trnddc08...
Roy

I make no claim to being qualified to discuss antennas with you when we
are in disagreement. I worked as an antenna design engineer for 15
years till 1968 when I was layed off from TRW. I was never a high level
theorist but managed to hold a decent position with designing hardware. I
did work with some highly qualified engineers from whom I thought I
obtained alot of knowledge about antennas. Thats why I was bold enough
to say "we". I still maintain a casual relationship with George Oltman
who you might know from his association with antenna groups with IEEE.
As for the F/B, I considered that to identify Front to Back of the
antenna's radiation pattern. I would consider it appropriate to identify
the radiation toward the "Front" as the max radiation to the front. Then,
it seems that the numerical level used for the "F/B ratio" should be max
to the Back.
I make no argument that this definition I use is *the* way F/B is. But,
dont we define "side lobe level" as the ratio of the main beam Max to the
side lobe Max? Be aware, I dont write to correct your thinking. I did
consider the F/B to be flawed when the main beam Max is compared with a
rear radiation Min.

I'll consider myself corrected and stop posting.

Jerry

"Roy Lewallen" wrote in message
...
What are "front" and "back"? If the maximum forward lobe is +10 dBi at an
elevation angle of 23 degrees and the best null is -30 dBi at an azimuth
angle 160 degrees from the peak forward lobe, and at an elevation angle
of 47 degrees, are you saying that by your definition the front/back
ratio is 40 dB? If so, I guess that's interesting but I can't imagine
what it might be good for.

Who's "we"?

Roy Lewallen, W7EL

Jerry Martes wrote:
Roy

When I was working with antennas, we considered the antenna's F/B
ratio used the max of the front compared to the max of the back. But,
I get the impression that the rules are different now.

Jerry






[email protected] April 5th 05 02:18 PM

I agree Roy, I did say it wasn't easy and I suspect you are correct if the
null is "deep"
But if the general" Front to rear"is exceptionaly good then
there is no reason for the F/B not to fairly accurate.
I certainly would not call it "silly" which is exactly
how "old wives tales" start.
The particular case I was referring to was where multiple
reflectors were used to dampen rearward radiation to a minimum.

Regards
Art




"Roy Lewallen" wrote in message
...
wrote:
. . .
I have seen computor results
that offer 50 db F/B based on NEC, Can I trust gain if F/B cannot
be trusted?


Absolutely! While you might get some very deep nulls at some particular
points in space, and fairly deep nulls in some particular
azimuth/elevation angle combinations, they're not likely to be exactly as
deep or in the directions the program reports. Gain, on the other hand,
can be strikingly accurate in many cases.

Put together any model you want with an extreme F/B ratio. Then fiddle the
model just slightly -- change the frequency, element length or diameter,
etc. Look at how much the gain changes, and how much the F/B changes.
Modify it more, and look again.

You'll see that the F/B is *much* more critical than gain. You can goof up
the model -- or real antenna -- a lot more without any appreciable change
in gain than you can before seeing major changes in F/B.

The reason is simple. To get a deep null and therefore good F/B ratio, you
have to add the fields from all parts of the antenna together to get zero
within a tiny, tiny fraction of a percent. If any one of the fields
changes just a tiny amount, they no longer sum precisely to zero. But
small change like that won't noticeably affect the gain. No model is good
enough to precisely predict extremely deep nulls -- there's always too
much difference between the model and reality.

I don't recall what Reg recently said, but I've gotten 50 dB and greater
F/B ratios from an array by adjusting the phasing network while listening
to a receiver placed in the null direction. But the null is that deep only
in that direction, at that height above ground. It's also noticeably
shallower a little ways away even in the same direction, because I've
compensated for re-radiation from nearby objects, too. Even coax shield
leakage becomes a very noticeable factor. So while I can tweak an array to
get a very deep null, there's no way I can expect that to hold when
anything changes, even just a little. I'd even expect it to change from
day to day as the ground moisture changes and the sap rises in the trees.

Obviously 50 db is hard to get but is it beyond the realms
of possibility?


For what, one particular azimuth/elevation combination at one single
frequency? You might be able to do it. But it would be only of academic
interest at best.

. . .


Roy Lewallen, W7EL




Richard Harrison April 5th 05 04:31 PM

Jerry Martes wrote:
"When I was working with antwennas, we considered the antenna`s F/B
ratio used the max of the front to the max of the back. But I get the
impression that the erules are different now."

Front-to-back ratio is defined as the ratio of power gain between front
and rear of a directional antenna.

A.W.P. King writes on page 209 of "Transision Lines, Antennas, and Wave
Guides"*:

"In practice, it is usually important to maximize the ratio of forward
to backward field or the ratio of backward to forward field. If the
ratio of forward to backward field is maximized, the parasite is called
a reflector; if the ratio of backward to forward field is maximized, the
parasite is called a director."

I don`t think the above has changed since 1945.

Best regards, Rihard Harrison, KB5WZI


[email protected] April 5th 05 04:53 PM

Richard
That rule is not all encompasing tho it may well suffice for yagi's and the
like
Regards
Art
"Richard Harrison" wrote in message
...
Jerry Martes wrote:
"When I was working with antwennas, we considered the antenna`s F/B
ratio used the max of the front to the max of the back. But I get the
impression that the erules are different now."

Front-to-back ratio is defined as the ratio of power gain between front
and rear of a directional antenna.

A.W.P. King writes on page 209 of "Transision Lines, Antennas, and Wave
Guides"*:

"In practice, it is usually important to maximize the ratio of forward
to backward field or the ratio of backward to forward field. If the
ratio of forward to backward field is maximized, the parasite is called
a reflector; if the ratio of backward to forward field is maximized, the
parasite is called a director."

I don`t think the above has changed since 1945.

Best regards, Rihard Harrison, KB5WZI




Richard Harrison April 5th 05 05:09 PM

Art Unwin wrote:
"The particular case I was referring to was where multiple reflectors
were used to dampen radiation to a maximum."

It works. Taken to an extreme, you have a grid-dish reflector.

Additional reflectors in the plane of the other Yagi-Uda elements don`t
make best use of materials aloft. Placed ahead of the driven element,
additional elements are in a strong field where they may work as
directors to sharpen the forward gain. Placed behind the reflector which
has already reversed most of the energy in its direction, a parasitic
element is less effective as rhere is less energy to work with.

Best regards, Richard Harrison, KB5WZI


Cecil Moore April 5th 05 05:16 PM

wrote:
I certainly would not call it "silly" which is exactly
how "old wives tales" start.


At first, Einstein thought quantum physics was silly
(spooky). Entangled particles violate the spirit of
Einstein's relativity, if not the letter (at least
not yet). :-)
--
73, Cecil
http://www.qsl.net/w5dxp

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[email protected] April 5th 05 06:38 PM


"Richard Harrison" wrote in message
...
Art Unwin wrote:
"The particular case I was referring to was where multiple reflectors
were used to dampen radiation to a maximum."

It works. Taken to an extreme, you have a grid-dish reflector.

Additional reflectors in the plane of the other Yagi-Uda elements don`t
make best use of materials aloft.


Generaly I can agree with that but it is NOT TRUE in all cases.

1 It can NEVER reflect all radiation from the rear
2 Coupling is reduced as the directors move away from the driven element
to the point where little current flows.!

A yagi does have an advantage in simplicity together with the ability
to "focus" the forward lobe but not at the expense of removing rearward
radiation.

This post is starting to be remoniscent of the old days where Guru's stated
that more
than one reflector was pointless and unproductive because they could only
think
Yagis to the ommission of all others . Need W8TI to complete the full circle
(On a prior post I brought up the corner reflector antenna but I had
temporarily forgotten
that the reflectors carried little current and thus could not be a good
contender
for high F/B)





Placed ahead of the driven element,
additional elements are in a strong field where they may work as
directors to sharpen the forward gain. Placed behind the reflector which
has already reversed most of the energy in its direction, a parasitic
element is less effective as rhere is less energy to work with.


HUM.... isn't F/B values retarded when maximum gain occurs?
This suggests that max gain occurs when there is MORE energy to
work with at the rear does it not?
Regards
Art

Best regards, Richard Harrison, KB5WZI




[email protected] April 6th 05 03:08 AM


"Richard Harrison" wrote in message
...
Art Unwin wrote:
"The particular case I was referring to was where multiple reflectors
were used to dampen radiation to a maximum."

It works. Taken to an extreme, you have a grid-dish reflector.




No, No, No Richard! I do not


A grid-dish reflector is where the reflector assembly has voids in the
reflector panel
that R.F. cannot penetrate. A similar instance is the perforations in a
transmitter housing.
Maybe it was the term "dampen" that led you to think I had a "grid" type
reflector which is not the case.
My antenna consists of 8 - 1/2 wave elements of which one is fed. All others
are resonant reflectors
set on a parabolic curve as is the driven element, thus it does not
"focus".This can be
fabricated using standard straight dipole elements . Advantages are to be
had using elements
that are "shaped" to minimise "reactance" coupling and also the physical
turning radius.
It is this variation that I am building now to see if it becomes quieter
especially when static is around.
It is times like this that light telescopic fishing poles can be used to
advantage together with
aluminum tubular mast. You may remember that I sent a 60 foot boom yagi
picture to you
years ago with 13 elements ( 26 fishing poles) which was also light weight
and thus desirable
when testing or experimenting to find out where the knoweledge envelope can
be pushed.
Regards
Art





Additional reflectors in the plane of the other Yagi-Uda elements don`t
make best use of materials aloft. Placed ahead of the driven element,
additional elements are in a strong field where they may work as
directors to sharpen the forward gain. Placed behind the reflector which
has already reversed most of the energy in its direction, a parasitic
element is less effective as rhere is less energy to work with.

Best regards, Richard Harrison, KB5WZI




Roy Lewallen April 6th 05 06:24 AM

Please don't consider yourself unqualified. I don't think anyone posting
on this newsgroup should, and with your background you certainly shouldn't.

My question about who "we" meant was to establish a context for the
definition you used, which you've supplied -- thanks.

The definition you use isn't a bad one, although it might not be the
most useful, provided that you restrict the analysis to free space and
are speaking only of a single plane of the 3D pattern. This is commonly
done in discussing Yagi arrays, for example. Perhaps your experience was
largely in Yagi, log periodic, or other planar arrays which lend
themselves to this simplification. The meaning of "back" is open to some
interpretation, though. Sometimes it means the precise direction that's
exactly 180 degrees from the main forward lobe. Sometimes, though, it
refers to a range of angles, even as great as the whole rear semicircle.
Let me give an example. Suppose an antenna nominally has a deep null
directly to the rear of the front lobe. But a slight asymmetry in the
antenna moves the lobe a few degrees to the side. This could easily
degrade a strictly defined ("rear" meaning exactly to the rear of the
peak of the front lobe) front/back ratio by 10 or 20 dB. It's hard to
conceive the application where it would really change the usefulness of
the antenna. But a very slightly asymmetrical antenna would look much
worse on paper. In your experience, would you consider this to be a poor
f/b ratio, or would you give the definition some slack and allow "rear"
to vary a few degrees? If you'd give it some slack, then the next
question is how much -- could the null be skewed 5 degrees? 10? more?

In my limited experience, when the second convention is used (allowing
the whole rear semicircle to count as "rear"), the "rear" figure often
comes from the largest lobe in the "rear" region. So the gain in the
precise direction opposite the front lobe doesn't matter, if there are
lobes in other directions in the rear semicircle. This definition would
be useful for amateur beam applications, because it tells you the
minimum amount of attenuation you'll get from signals coming from any
direction within the rear 180 degrees of the pattern. Who cares that you
have a 50 dB null in one very narrow direction, if a few degrees away
the response is 40 or 50 dB greater. The definition of front/back ratio
seems flexible, sometimes used to make the measure more meaningful or
useful, but sometimes, I'm sure, to obscure the quality of the pattern.

In the example I mentioned in my earlier posting, though, of the complex
pattern of an antenna over ground, the definition can get muddy indeed.
So it's often necessary to carefully define the term and state exactly
what you mean if you really want to communicate meaningful information
when you quote a "front/back" ratio.

Roy Lewallen, W7EL

Jerry Martes wrote:
Roy

I make no claim to being qualified to discuss antennas with you when we
are in disagreement. I worked as an antenna design engineer for 15 years
till 1968 when I was layed off from TRW. I was never a high level theorist
but managed to hold a decent position with designing hardware. I did work
with some highly qualified engineers from whom I thought I obtained alot of
knowledge about antennas. Thats why I was bold enough to say "we". I
still maintain a casual relationship with George Oltman who you might know
from his association with antenna groups with IEEE.
As for the F/B, I considered that to identify Front to Back of the
antenna's radiation pattern. I would consider it appropriate to identify
the radiation toward the "Front" as the max radiation to the front. Then,
it seems that the numerical level used for the "F/B ratio" should be max to
the Back.
I make no argument that this definition I use is *the* way F/B is. But,
dont we define "side lobe level" as the ratio of the main beam Max to the
side lobe Max? Be aware, I dont write to correct your thinking. I did
consider the F/B to be flawed when the main beam Max is compared with a rear
radiation Min.

I'll consider myself corrected and stop posting.

Jerry


Cecil Moore April 6th 05 05:11 PM

Cecil Moore wrote:
John Smith wrote:
I cannot find a configuration on the gamma which brings the swr under
that figure...


As Richard H. said, find the point where the feedpoint
resistance is 50 + jXL ohms. That must occur somewhere.
Then tune out the reactance with a series capacitor.


I've used EZNEC to model a gamma-fed 33' 20m dipole at
40' made out of 0.5" aluminum tubing. With a gamma element
three feet long 6" below the 33' element and a series
Xc=122 ohms, it indicates a feedpoint impedance of
49+j0.3 ohms. The EZNEC file can be downloaded by
clicking on the link below.
--
73, Cecil http://www.qsl.net/w5dxp/GAM20DIP.EZ


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John Smith April 6th 05 05:33 PM

Cecil:

Your work with EZNEC is greatly appreciated here.
Your configuration is for a horz ant and I am working with a
vertical--conversion is trivial.
"A picture is worth a thousand words..." has real significance here.
I am sure an analysis of your file will provide me with insight into the
workings of EZNEC and accelerate my learning curve!

THANKS!,
John

--
I would like to point out, I do appreciate the "Been there--done that!"
posts. Indeed, now your observations, comments and discourse should be
filled with wisdom--I am listening!!!
"Cecil Moore" wrote in message
...
Cecil Moore wrote:
John Smith wrote:
I cannot find a configuration on the gamma which brings the swr under
that figure...


As Richard H. said, find the point where the feedpoint
resistance is 50 + jXL ohms. That must occur somewhere.
Then tune out the reactance with a series capacitor.


I've used EZNEC to model a gamma-fed 33' 20m dipole at
40' made out of 0.5" aluminum tubing. With a gamma element
three feet long 6" below the 33' element and a series
Xc=122 ohms, it indicates a feedpoint impedance of
49+j0.3 ohms. The EZNEC file can be downloaded by
clicking on the link below.
--
73, Cecil http://www.qsl.net/w5dxp/GAM20DIP.EZ


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Cecil Moore April 6th 05 07:42 PM

John Smith wrote:
Your work with EZNEC is greatly appreciated here.
Your configuration is for a horz ant and I am working with a
vertical--conversion is trivial.
"A picture is worth a thousand words..." has real significance here.
I am sure an analysis of your file will provide me with insight into the
workings of EZNEC and accelerate my learning curve!


I knew I was confused about what you were trying to do.
If you just tilt the horizontal dipole to a vertical
position, it will still be center-fed. Are you trying
to gamma-match a 1/2WL vertical base-fed against a
radial system? If so, try this EZNEC file:
--
73, Cecil http://www.qsl.net/w5dxp/GAM20VHW.EZ

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Cecil Moore April 6th 05 08:28 PM

Cecil Moore wrote:
I knew I was confused about what you were trying to do.


John, I just realized what is wrong with gamma feeding a
1/2WL vertical at the base. The currents in each side of
the gamma feed section are pretty much out-of-phase so
they don't radiate (much). Conclusion: Gamma feeding a
1/2WL antenna at the base results in a field strength
comparable to a 1/4WL vertical and the minuscule amount
of gain is not worth the effort. Antenna gurus probably
already knew that but it just dawned on my concrete brain.

In much the same way a Zepp or a J-Pole is not a 3/4WL
radiator even though they are 3/4WL long, a gamma match
on a base-fed 1/2WL vertical doesn't yield a 1/2WL
electrical radiator. For this reason, the length of a
gamma match should be considerably less than a wavelength.
A good rule of thumb is probably in the ballpark of less
than ~6% of a wavelength. Your idea seems to require about
16% of a wavelength.

Moral: Physical length and RF electrical length are not
always the same.

What you are trying to do apparently requires a J-Pole
or Zepp approach, i.e. a physical 3/4WL antenna.
--
73, Cecil http://www.qsl.net/w5dxp

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John Smith April 6th 05 08:45 PM

Cecil:

One element I do not understand in EZNEC is: say I end up with 225 ohms
inductive reactance in the gamma rod(just an example figure, use any you
please), how do I inform EZNEC I am inserting a 225 ohm capactive reactance,
at the feedpoint to offset it?
Or, I am all wet in considering this?

Regards,
John

--
I would like to point out, I do appreciate the "Been there--done that!"
posts. Indeed, now your observations, comments and discourse should be
filled with wisdom--I am listening!!!
"John Smith" wrote in message
...
Cecil:

Your work with EZNEC is greatly appreciated here.
Your configuration is for a horz ant and I am working with a
vertical--conversion is trivial.
"A picture is worth a thousand words..." has real significance here.
I am sure an analysis of your file will provide me with insight into the
workings of EZNEC and accelerate my learning curve!

THANKS!,
John

--
I would like to point out, I do appreciate the "Been there--done that!"
posts. Indeed, now your observations, comments and discourse should be
filled with wisdom--I am listening!!!
"Cecil Moore" wrote in message
...
Cecil Moore wrote:
John Smith wrote:
I cannot find a configuration on the gamma which brings the swr under
that figure...

As Richard H. said, find the point where the feedpoint
resistance is 50 + jXL ohms. That must occur somewhere.
Then tune out the reactance with a series capacitor.


I've used EZNEC to model a gamma-fed 33' 20m dipole at
40' made out of 0.5" aluminum tubing. With a gamma element
three feet long 6" below the 33' element and a series
Xc=122 ohms, it indicates a feedpoint impedance of
49+j0.3 ohms. The EZNEC file can be downloaded by
clicking on the link below.
--
73, Cecil http://www.qsl.net/w5dxp/GAM20DIP.EZ


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John Smith April 6th 05 09:06 PM

Cecil:
Yes Cecil, there is wisdom in your words...
However, as I pointed out, I am now focusing on "received signal", its'
quality and strength.
After having given it some thought, that is what is most important. In an
grave emergency I have the ability to bring multiple kilowatts on line (yes,
I have the generator to support it.) What I can't do is guarantee that for
the fellow at the other end of the contact. So, I am focusing my attention
towards his/her benefit--in the refinement of my ability to pull
sub-nano-watts from the ether...
EZNEC and all other calculations are great, I appreciate what can get me to
ballpark figures with matching, lengths, spacings, predictions, etc.
But, in the end, the humble s-meter on a known transceiver, compared against
know signals and similar conditions will be my final guide and the
determining factor.
To all which point out I "may only be"/am duplicating past work, while
making futile attempts, or expelling great amounts of energy in this
pursuit, I say: "It keeps me out of the bars and away from the wild women!"
(saves on my Jim Beam/Viagra bill too!)

Warmest regards,
John

--
I would like to point out, I do appreciate the "Been there--done that!"
posts. Indeed, now your observations, comments and discourse should be
filled with wisdom--I am listening!!!
"Cecil Moore" wrote in message
...
Cecil Moore wrote:
I knew I was confused about what you were trying to do.


John, I just realized what is wrong with gamma feeding a
1/2WL vertical at the base. The currents in each side of
the gamma feed section are pretty much out-of-phase so
they don't radiate (much). Conclusion: Gamma feeding a
1/2WL antenna at the base results in a field strength
comparable to a 1/4WL vertical and the minuscule amount
of gain is not worth the effort. Antenna gurus probably
already knew that but it just dawned on my concrete brain.

In much the same way a Zepp or a J-Pole is not a 3/4WL
radiator even though they are 3/4WL long, a gamma match
on a base-fed 1/2WL vertical doesn't yield a 1/2WL
electrical radiator. For this reason, the length of a
gamma match should be considerably less than a wavelength.
A good rule of thumb is probably in the ballpark of less
than ~6% of a wavelength. Your idea seems to require about
16% of a wavelength.

Moral: Physical length and RF electrical length are not
always the same.

What you are trying to do apparently requires a J-Pole
or Zepp approach, i.e. a physical 3/4WL antenna.
--
73, Cecil http://www.qsl.net/w5dxp

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Jim Kelley April 6th 05 09:34 PM



John Smith wrote:

Cecil:
Yes Cecil, there is wisdom in your words...
However, as I pointed out, I am now focusing on "received signal", its'
quality and strength.
After having given it some thought, that is what is most important. In an
grave emergency I have the ability to bring multiple kilowatts on line (yes,
I have the generator to support it.) What I can't do is guarantee that for
the fellow at the other end of the contact. So, I am focusing my attention
towards his/her benefit--in the refinement of my ability to pull
sub-nano-watts from the ether...
EZNEC and all other calculations are great, I appreciate what can get me to
ballpark figures with matching, lengths, spacings, predictions, etc.
But, in the end, the humble s-meter on a known transceiver, compared against
know signals and similar conditions will be my final guide and the
determining factor.


I think you'll eventually end up finding out you just need a big tower
and a big beam.

ac6xg




Richard Harrison April 6th 05 11:04 PM

Roy, W7EL wrote:
"Who cares that you have a 50 dB null in one particular very narrow
direction, if a few degrees away the response is 40 or 50 dB greater."

This is an example of Roy`s earlier post which noted differences between
amateur requirements and commercial requirements. Roy is right. There
are real differences.

Commercial licensees operate on assigned frequencies and enjoy some
protection from interference on their assignments. A broadcaster may as
a condition of his license be required to have a null in one or more
azimuths in his pattern to protect another broadcaster who was there
first. In this broadcaster`s case, he is interested in the narrow null
and may very well expect and hope his signal a few dgrees away is 40 or
50 dB greater.

Best regards, Richard Harrison, KB5WZI


John Smith April 6th 05 11:13 PM

Hmmmm, your analysis is interesting. The gamma looks very much like an
"auto-transformer" to me--the gama-rod like a variable primary, the
secondary being the complete driven element.
I suspected the action would be identical to the auto-transformer--where ALL
the turns in the secondary deliver power to the load....

Regards,
John


--
I would like to point out, I do appreciate the "Been there--done that!"
posts. Indeed, now your observations, comments and discourse should be
filled with wisdom--I am listening!!!
"Cecil Moore" wrote in message
...
Cecil Moore wrote:
I knew I was confused about what you were trying to do.


John, I just realized what is wrong with gamma feeding a
1/2WL vertical at the base. The currents in each side of
the gamma feed section are pretty much out-of-phase so
they don't radiate (much). Conclusion: Gamma feeding a
1/2WL antenna at the base results in a field strength
comparable to a 1/4WL vertical and the minuscule amount
of gain is not worth the effort. Antenna gurus probably
already knew that but it just dawned on my concrete brain.

In much the same way a Zepp or a J-Pole is not a 3/4WL
radiator even though they are 3/4WL long, a gamma match
on a base-fed 1/2WL vertical doesn't yield a 1/2WL
electrical radiator. For this reason, the length of a
gamma match should be considerably less than a wavelength.
A good rule of thumb is probably in the ballpark of less
than ~6% of a wavelength. Your idea seems to require about
16% of a wavelength.

Moral: Physical length and RF electrical length are not
always the same.

What you are trying to do apparently requires a J-Pole
or Zepp approach, i.e. a physical 3/4WL antenna.
--
73, Cecil http://www.qsl.net/w5dxp

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John Smith April 6th 05 11:51 PM

Cecil:

Maybe I sent you the wrong .EZ file.
Anyway, I went back and pondered over your example, DUH!, it was obivious, I
simply had to splilt the driven element into two sections where the gamma
joined it!

Oh well, I might have made myself look stupid today, but not to such a great
extent that I won't be able to top that tomorrow!!!

Regards,
John

--
I would like to point out, I do appreciate the "Been there--done that!"
posts. Indeed, now your observations, comments and discourse should be
filled with wisdom--I am listening!!!
"John Smith" wrote in message
...
Cecil:

Here is an EZNEC file I am having a problem with, it is complaining about
wires 5 and 2 NOT meeting at an end or segment?
What corrects this?

Thanks in advance,
warmest regards,
John


--
I would like to point out, I do appreciate the "Been there--done that!"
posts. Indeed, now your observations, comments and discourse should be
filled with wisdom--I am listening!!!
"Cecil Moore" wrote in message
...
Cecil Moore wrote:
I knew I was confused about what you were trying to do.


John, I just realized what is wrong with gamma feeding a
1/2WL vertical at the base. The currents in each side of
the gamma feed section are pretty much out-of-phase so
they don't radiate (much). Conclusion: Gamma feeding a
1/2WL antenna at the base results in a field strength
comparable to a 1/4WL vertical and the minuscule amount
of gain is not worth the effort. Antenna gurus probably
already knew that but it just dawned on my concrete brain.

In much the same way a Zepp or a J-Pole is not a 3/4WL
radiator even though they are 3/4WL long, a gamma match
on a base-fed 1/2WL vertical doesn't yield a 1/2WL
electrical radiator. For this reason, the length of a
gamma match should be considerably less than a wavelength.
A good rule of thumb is probably in the ballpark of less
than ~6% of a wavelength. Your idea seems to require about
16% of a wavelength.

Moral: Physical length and RF electrical length are not
always the same.

What you are trying to do apparently requires a J-Pole
or Zepp approach, i.e. a physical 3/4WL antenna.
--
73, Cecil http://www.qsl.net/w5dxp

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Dave April 7th 05 12:00 AM

have you tried this???
http://www.google.com/search?hl=en&q...ch+yagi+design
lots of sources for design info, some software, plenty of pointers.
basically once you have a yagi and decide to feed it with a gamma match you
have the following variables you can work with (assuming you aren't going
to change the diameter of the driven element)...
1. rod diameter
2. rod to driven element spacing
3. location of shorting strap
4. value of capacitance
5. length of driven element(don't forget this, it is very important part of
adjustment!)

now basically you pick a rod diameter, usually 1/3 to 1/2 the diameter of
the driven element, but basically whatever you happen to have handy that is
a reasonable length. then make a few brackets to space it a couple inches
from the driven element, from about 1" on 2m to maybe 4-5" on 20m. so that
fixes 1 and 2.. then you have 3 other variables you can adjust to get the
match you want. if you can't find a good match after systematically running
through the other 3 then try changing the spacing a bit and start again...
but i've always been able to get a decent match by just picking what was
handy for tubing and spacers.

and don't overlook a T match. if you use a 1/2 wave phasing line and the
right diameters and spacing you can get away without a capacitor. this
makes for a fully dc grounded plumbers delight construction that is very
rugged and simple to adjust. this was how all the old telrex monobanders
were fed.



"Jim Kelley" wrote in message
...


John Smith wrote:

Cecil:
Yes Cecil, there is wisdom in your words...
However, as I pointed out, I am now focusing on "received signal", its'
quality and strength.
After having given it some thought, that is what is most important. In

an
grave emergency I have the ability to bring multiple kilowatts on line

(yes,
I have the generator to support it.) What I can't do is guarantee that

for
the fellow at the other end of the contact. So, I am focusing my

attention
towards his/her benefit--in the refinement of my ability to pull
sub-nano-watts from the ether...
EZNEC and all other calculations are great, I appreciate what can get me

to
ballpark figures with matching, lengths, spacings, predictions, etc.
But, in the end, the humble s-meter on a known transceiver, compared

against
know signals and similar conditions will be my final guide and the
determining factor.


I think you'll eventually end up finding out you just need a big tower
and a big beam.

ac6xg






John Smith April 7th 05 01:41 AM

Cecil:

Here is the crux of my fruitless attempts to use EZNEC...
With EZNEC, when I plug in the value of my gamma rod and -jxr, along with
all other elements, EZNEC spits out an error! (something about too short a
loop seems to bother EZNEC, but this short loop IS working!)
However, I am looking at a REAL and functional antenna which appears to be
well matched and receiving well.
So, I end up throwing up my hands and just using the antenna and going about
with the "cut-and-try" method! (probably just my inability to use the app)

Regards,
John
--
I would like to point out, I do appreciate the "Been there--done that!"
posts. Indeed, now your observations, comments and discourse should be
filled with wisdom--I am listening!!!
"John Smith" wrote in message
...
Cecil:

One element I do not understand in EZNEC is: say I end up with 225 ohms
inductive reactance in the gamma rod(just an example figure, use any you
please), how do I inform EZNEC I am inserting a 225 ohm capactive
reactance,
at the feedpoint to offset it?
Or, I am all wet in considering this?

Regards,
John

--
I would like to point out, I do appreciate the "Been there--done that!"
posts. Indeed, now your observations, comments and discourse should be
filled with wisdom--I am listening!!!
"John Smith" wrote in message
...
Cecil:

Your work with EZNEC is greatly appreciated here.
Your configuration is for a horz ant and I am working with a
vertical--conversion is trivial.
"A picture is worth a thousand words..." has real significance here.
I am sure an analysis of your file will provide me with insight into the
workings of EZNEC and accelerate my learning curve!

THANKS!,
John

--
I would like to point out, I do appreciate the "Been there--done that!"
posts. Indeed, now your observations, comments and discourse should be
filled with wisdom--I am listening!!!
"Cecil Moore" wrote in message
...
Cecil Moore wrote:
John Smith wrote:
I cannot find a configuration on the gamma which brings the swr under
that figure...

As Richard H. said, find the point where the feedpoint
resistance is 50 + jXL ohms. That must occur somewhere.
Then tune out the reactance with a series capacitor.

I've used EZNEC to model a gamma-fed 33' 20m dipole at
40' made out of 0.5" aluminum tubing. With a gamma element
three feet long 6" below the 33' element and a series
Xc=122 ohms, it indicates a feedpoint impedance of
49+j0.3 ohms. The EZNEC file can be downloaded by
clicking on the link below.
--
73, Cecil http://www.qsl.net/w5dxp/GAM20DIP.EZ


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Richard Harrison April 7th 05 06:09 AM

John Smith wrote:
"However, I am looking at a REAL and functional antenna which appears to
be well matched and receiving well."

Congratulationns!

In a previous posting, I quoted Dr. Arnold King who wrote prior to 1945:
"The accurate calculation of the (antenna) input impedance at AB of the
modified antenna as a function of the impedance (presented to the
matching section) and the (wire) lengths AC and BD has not been
accomplished."

If it were easy to calculate, they would have done it. They had
excellent marhematicians prior to 1945, too. The implication is that you
find the match by trial. John proved he could do it.

Best regards, Richard Harrison, KB5WZI


Cecil Moore April 7th 05 02:23 PM

John Smith wrote:
Cecil:

One element I do not understand in EZNEC is: say I end up with 225 ohms
inductive reactance in the gamma rod(just an example figure, use any you
please), how do I inform EZNEC I am inserting a 225 ohm capactive reactance,
at the feedpoint to offset it?


Use the "Loads" feature to install a lumped point load of
any Q. For instance, a coil might be 10 + j300 ohms or
a cap might be 2 - j500 ohms. The position of a load
is similar to positioning a source.
--
73, Cecil http://www.qsl.net/w5dxp

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Cecil Moore April 7th 05 02:35 PM

John Smith wrote:

Cecil:

Maybe I sent you the wrong .EZ file.
Anyway, I went back and pondered over your example, DUH!, it was obivious, I
simply had to splilt the driven element into two sections where the gamma
joined it!

Oh well, I might have made myself look stupid today, but not to such a great
extent that I won't be able to top that tomorrow!!!


I dare say all of us EZNEC users have committed that infraction,
some more than once. :-)
--
73, Cecil http://www.qsl.net/w5dxp

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Cecil Moore April 7th 05 03:22 PM

John Smith wrote:

Cecil:

Here is the crux of my fruitless attempts to use EZNEC...
With EZNEC, when I plug in the value of my gamma rod and -jxr, along with
all other elements, EZNEC spits out an error! (something about too short a
loop seems to bother EZNEC, but this short loop IS working!)
However, I am looking at a REAL and functional antenna which appears to be
well matched and receiving well.
So, I end up throwing up my hands and just using the antenna and going about
with the "cut-and-try" method! (probably just my inability to use the app)


Or maybe not. EZNEC apparently won't properly model
the Lattin antenna. www.g3ycc.karoo.net/lattin.htm

Somewhere I have a .ez file that shows 20 dBi omni-
directional gain from an inverted-L antenna. Now that's
what you need. :-)

And you taught me something today. I didn't know one
can attach .ez files to a newsgroup posting.
--
73, Cecil http://www.qsl.net/w5dxp

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Richard Harrison April 7th 05 04:06 PM

Cecil Moore, W5DXP wrote:
"For instance, a coil might be 10+j300 ohms or a cap might be 2-j500
ohms."

A small loop antenna with a perimeter only a small fraction of a
wavelength has almost uniform current throughout. Its impedance is an
inductive reactance in series with a resistance. The U.S. Bureau of
Standards published inductance formulas for single-turn and several-turn
loops in Bulletin 74. Results can`t take into account loss from
radiation so they are approximate.

Arnold King gives an approximate formula for the radiation resistance of
a small one-turn loop in "Transmission Lines, Antennas, and Wave
Guides":
Re = 20(Beta)to the 4th power times A squared
Beta=2pi/lambda
A=area enclosed by the loop.

Best regards, Richard Harrison, KB5WZI


Roy Lewallen April 7th 05 06:05 PM

Cecil Moore wrote:

Or maybe not. EZNEC apparently won't properly model
the Lattin antenna. www.g3ycc.karoo.net/lattin.htm
. . .


I took a look at it, and sure enough, it can't. The antenna is
constructed from tubular 300 ohm twinlead, and EZNEC has no way to
account for the dielectric between conductors. In that antenna, it looks
like the velocity factor of the differential mode field between
conductors would be important to its operation, and without the ability
to model the dielectric between conductors, EZNEC wouldn't get the
velocity factor right.

When I see a claim that EZNEC can't model a particular antenna, I often
find that the reason for the claim is that the antenna's inventor or
seller has dreamed up some magical property to explain the impossibly
good performance he's claiming for the antenna. EZNEC models the antenna
just fine, it just doesn't model the magical property and validate the
claims -- that is, it shows how the antenna really works, not how the
huckster claims it works. But there are, certainly, some kinds of
antennas which it really can't model properly for one reason or another.
The Lattin antenna is one of those.

Roy Lewallen, W7EL

Richard Clark April 7th 05 07:52 PM

On Thu, 07 Apr 2005 10:05:04 -0700, Roy Lewallen
wrote:

But there are, certainly, some kinds of
antennas which it really can't model properly for one reason or another.
The Lattin antenna is one of those.


Hi Roy,

Having model dozens of variations of this antenna, as well as what was
described in the patent - I cannot think of one reason why it should
work except through haphazard luck. Certainly the offered "theories"
are no more credible than those for other antennas that defy modeling
such as the single or double bazooka, the eh, the cfa.

This antenna has many reports of its confounding expectation and then
in the same breath those who are confounded expressing their sincere
belief it works. It's one of those situations where the builder can't
get it to sing, but has a brother-in-law who knows this fellow who
lives next door to one who can, but who took it down ten years ago
because it was so hard to tune.

Perhaps you could widen your customer base if you added a "belief
scale" to the available control settings for EZNEC. It could range
from "agnostic" to "I believe in miracles."

73's
Richard Clark, KB7QHC

Cecil Moore April 7th 05 09:18 PM

John Smith wrote:

Cecil:

Take a look at this folded wave monopole...
I am playing with a reflector and director to sandwich this driven element
between....
This is the design I have in mind, NO groundplane radials when used as a
stand-alone vertical monopole/end-fed.


There are warnings in EZNEC about segments not lining up
between close spaced wires. My 29 dBi omnidirectional
antenna is an example of what happens when one ignores
the segment alignment between closely spaced segments.

I have modified your segmentation to try to follow the
EZNEC guidelines and that file is attached. There is
quite a change in the results. The feedpoint impedance
went from 2.787+j15.47 to 0.7587+j22.69, the gain went
from 7.23 dBi to 3.16 dBi, and the TOA went from 6 deg
to 9 deg. I standardized on one foot per segment.

I don't really understand what you are trying to do and
am just the messenger.
--
73, Cecil http://www.qsl.net/w5dxp

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John Smith April 7th 05 10:03 PM

Cecil:

Did you remember to attach the file? I don't see it, but would love to
study your changes...
At ~2.7 ohms I can use a 1:16 balun (reversed direction from conventional
use) to mate the antenna with 50 ohms, and get an acceptable SWR...
Cecil, try to hear this in a positive manner: If I must conform to EZNEC,
then any creativity must be abandoned... If I conform to all the rules of
the past and the "Absolute Truths" encompassed by any application--how could
I ever hope for a new discovery of geometry or configuration, or the
possible use of un-used manipulations of existing rules?
If one travels the same road, takes the same plane, rides the same rail,
boards the same boat, walks the same path--he sees only the same sights,
that which is common place.... even futile paths invoke my curriosity--as
just a change of scenery can be enjoyed many times.
If that argument is carried out to its nth degree, only one question would
remain, "Why should I bother with any of this?", it would be quite easy for
a programmer to create a program which quizzes you on ant type (monopole,
dipole, yagi, 1/2 wave, 1/4 wave, center loaded, bottom loaded, etc, etc),
the freq etc... then constructs the antenna for you. Including suggesting
height, mounting brackets and a host of other varibles and conditions that
tasks the mind to consider... In other words, once I give control and
authority to EZNEC, why should it not "do it all?"
But then, even if it did, I would still dilly around with these copper,
aluminum and stainless bits and pieces. grin
You have talked me back into abandoning EZNEC....

Regards,
John

--
I would like to point out, I do appreciate the "Been there--done that!"
posts. Indeed, now your observations, comments and discourse should be
filled with wisdom--I am listening!!!
"Cecil Moore" wrote in message
...
John Smith wrote:

Cecil:

Take a look at this folded wave monopole...
I am playing with a reflector and director to sandwich this driven
element
between....
This is the design I have in mind, NO groundplane radials when used as a
stand-alone vertical monopole/end-fed.


There are warnings in EZNEC about segments not lining up
between close spaced wires. My 29 dBi omnidirectional
antenna is an example of what happens when one ignores
the segment alignment between closely spaced segments.

I have modified your segmentation to try to follow the
EZNEC guidelines and that file is attached. There is
quite a change in the results. The feedpoint impedance
went from 2.787+j15.47 to 0.7587+j22.69, the gain went
from 7.23 dBi to 3.16 dBi, and the TOA went from 6 deg
to 9 deg. I standardized on one foot per segment.

I don't really understand what you are trying to do and
am just the messenger.
--
73, Cecil http://www.qsl.net/w5dxp

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John Smith April 9th 05 04:32 PM

Richard H:

Do you happen to have a URL handy where I could view "Bulletin 74?"

Thanks in advance,
warmest regards,
John

--
I would like to point out, I do appreciate the "Been there--done that!"
posts. Indeed, now your observations, comments and discourse should be
filled with wisdom--I am listening!!!
"Richard Harrison" wrote in message
...
Cecil Moore, W5DXP wrote:
"For instance, a coil might be 10+j300 ohms or a cap might be 2-j500
ohms."

A small loop antenna with a perimeter only a small fraction of a
wavelength has almost uniform current throughout. Its impedance is an
inductive reactance in series with a resistance. The U.S. Bureau of
Standards published inductance formulas for single-turn and several-turn
loops in Bulletin 74. Results can`t take into account loss from
radiation so they are approximate.

Arnold King gives an approximate formula for the radiation resistance of
a small one-turn loop in "Transmission Lines, Antennas, and Wave
Guides":
Re = 20(Beta)to the 4th power times A squared
Beta=2pi/lambda
A=area enclosed by the loop.

Best regards, Richard Harrison, KB5WZI




Richard Harrison April 10th 05 05:39 AM

John Smith wrote:
"Do you happen to have a URL handy where I could view "Bulletin 74?"

I searched the web unsuccessfully, including some NIST sites which
dictated schedules for clearing their files at certain file ages. But, I
did find a reference to the famous bulletin in Keith Henney`s 1950
edition of "Radio Engineering Handbook". On page 132, Keith writes:
"It is possible to calculate the true (l-f) inductance of some types of
air-cored coils with a fair degree of accuracy. National Bureau of
Standards Circular 74 has long been the most authorative source of such
information. Some of the most useful contained therein are reproduced
here."

Pages of information follow which include design charts which I can`t
reproduce due to my limitations. Such information is not copyrighted as
it is assumed the taxpayer has paid for collection of the information
already, and should not have to pay for it a second time. That was pre
Bush policy, of course.

You can probably borrow a copy of Keith Henney`s book in a library near
you and delight ijn designing your own antenna coil. The publisher was
McGraw-Hill.

Best regards, Richard Harrison, KB5WZI


Richard Clark April 10th 05 08:23 AM

On Sat, 9 Apr 2005 23:39:15 -0500, (Richard
Harrison) wrote:

National Bureau of
Standards Circular 74 has long been the most authorative source of such
information. Some of the most useful contained therein are reproduced
here."


Hi Richard,

Some background material:
"George Southworth was born in Little Cooley, Pennsylvania, in
1890 and became interested in radio while still in high school. He
graduated with a degree in physics from Grove City College in 1914
and then studied for a year at Columbia University. In June 1917
he joined the Radio Section of the U.S. National Bureau of
Standards and assisted in the preparation of the influential
Bulletin 74 entitled Radio Instruments and Measurements, published
in1918.
... [some time later]
"In 1931 he began a study of wave propagation in dielectric rods,
although the project did not yet have official authorization. By
early 1932, he observed wave propagation in a water-filled copper
pipe. Theoretical analysis related to Southworth's experiments was
carried out by John R. Carson, Sergei A. Schelkunoff, and Sallie
P. Mead during 1932.
"Using high-frequency vacuum tubes imported from France,
Southworth transmitted waves through air-filled copper pipes up to
20 feet long by May 1933. He later recalled that the first message
sent through a waveguide was 'Send money.'"

73's
Richard Clark, KB7QHC

Richard Clark April 10th 05 09:10 AM

On Sat, 9 Apr 2005 23:39:15 -0500, (Richard
Harrison) wrote:

I searched the web unsuccessfully

http://www.hills2.u-net.com/private/...4/CONTENTS.HTM
contains partial page transcriptions.

Employing the search term "Radio Instruments and Measurements" at:
http://www.kartoo.com/
you can make use of an unique, cluster based search engine that
represents the next wave of sifting information on the Web.

You will find references to this tome (hardly a circular or bulletin)
of more than 600 pages (you will also find book venders ready to sell
this work for $20-$30). One NIST site contains a quote from Edison:
" . . . This is the greatest book on this subject that I have ever
read, and I want to congratulate you and your Bureau on its
production."

There are multiple authors. I cited one, George Clark Southworth,
another was J. Howard Dellinger.

There are hard copies available through NIST's Historical Archives
(try to get one though).

73's
Richard Clark, KB7QHC

John Smith April 10th 05 04:04 PM

Richard:

Could these be them; or, are these not the same?

http://www.fcc.gov/mb/audio/decdoc/r...bulletins.html

Regards
--
I would like to point out, I do appreciate the "Been there--done that!"
posts. Indeed, now your observations, comments and discourse should be
filled with wisdom--I am listening!!!
"Richard Clark" wrote in message
...
On Sat, 9 Apr 2005 23:39:15 -0500, (Richard
Harrison) wrote:

I searched the web unsuccessfully

http://www.hills2.u-net.com/private/...4/CONTENTS.HTM
contains partial page transcriptions.

Employing the search term "Radio Instruments and Measurements" at:
http://www.kartoo.com/
you can make use of an unique, cluster based search engine that
represents the next wave of sifting information on the Web.

You will find references to this tome (hardly a circular or bulletin)
of more than 600 pages (you will also find book venders ready to sell
this work for $20-$30). One NIST site contains a quote from Edison:
" . . . This is the greatest book on this subject that I have ever
read, and I want to congratulate you and your Bureau on its
production."

There are multiple authors. I cited one, George Clark Southworth,
another was J. Howard Dellinger.

There are hard copies available through NIST's Historical Archives
(try to get one though).

73's
Richard Clark, KB7QHC





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