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Richard Fry June 11th 04 01:23 PM

Non-radiating Feedlines?
 
Post below from May 20, 2004

Wouldn't a "non-radiating" feedline in the field of a radiator also distort
the patterns of that radiator? Any conductor can do that, even if it is not
a feedline. NEC-2 models of FM broadcast transmit elements (and test range
patterns) show this clearly.

Paper 6 at http://rfry.org shows the free space patterns that the element
arms of a rototiller FM broadcast transmit antenna develop if they could be
driven from internal power sources -- and then the effects of adding the
element stem, mounts, feedline, and some nearby tower structure. The
patterns can get very skewed, even though the only radiators getting power
via a metallic path from the tx are the element arms themselves.

RF
____________

"Roy Lewallen" wrote
With a typical ground plane antenna, the feedline can radiate
significantly, distorting the pattern. This effect could easily be
different for the different antennas. Modeling indicates that two baluns
are often needed to suppress the current on the outside of the feedline.
A model which includes the feedline might give some insights as to why
the antennas behave so differently.




Roy Lewallen June 11th 04 07:31 PM

No.

A "non-radiating" feedline is one on which there is no net current
(i.e., no common mode current). In the case of coax, this translates to
zero current on the outside of the shield; for twinlead feedlines, it
means that the currents in the two conductors are exactly equal in
magnitude and opposite in direction.

Pattern distortion is caused by current being induced in a conductor by
an impinging field. That current, in turn, creates a field which adds to
the impinging field, resulting in pattern distortion. (This is, in fact,
the way a Yagi functions.) If there is current induced in a feedline by
the field, it's a radiating conductor (because the current causes
radiation which interferes with the impinging field). If there is no
current induced in the feedline by the impinging field, it creates no
field of its own (i.e., it's non-radiating) and therefore causes no
interference.

A transmission line placed symmetrically with respect to a dipole won't
have any current induced in it, although current can be conducted via a
direct connection. A transmission line asymmetrically placed will have
current induced in it and will distort the pattern. The feedline of a
ground plane or J-Pole likewise has induced current which distorts the
pattern. The amount of common mode current flowing in a transmission
line can be reduced by introducing an impedance to the common mode
current. It's desirable to do this without disturbing the differential
mode transmission line operation. That's the function of a balun. The
amount of induced current depends strongly on the orientation and length
of the parasitic conductor, and might be large or small in a particular
case.

Roy Lewallen, W7EL

Richard Fry wrote:
Post below from May 20, 2004

Wouldn't a "non-radiating" feedline in the field of a radiator also distort
the patterns of that radiator? Any conductor can do that, even if it is not
a feedline. NEC-2 models of FM broadcast transmit elements (and test range
patterns) show this clearly.

Paper 6 at http://rfry.org shows the free space patterns that the element
arms of a rototiller FM broadcast transmit antenna develop if they could be
driven from internal power sources -- and then the effects of adding the
element stem, mounts, feedline, and some nearby tower structure. The
patterns can get very skewed, even though the only radiators getting power
via a metallic path from the tx are the element arms themselves.

RF
____________

"Roy Lewallen" wrote

With a typical ground plane antenna, the feedline can radiate
significantly, distorting the pattern. This effect could easily be
different for the different antennas. Modeling indicates that two baluns
are often needed to suppress the current on the outside of the feedline.
A model which includes the feedline might give some insights as to why
the antennas behave so differently.





Richard Fry June 11th 04 09:04 PM

A balun can reduce common mode feedline currents due to the power supplied
to the line by the transmitter, but if the feedline is immersed in an
asymmetric radiated field, how does the balun reduce/remove the resulting,
unpredictable differential current on the feedline, and its contribution
toward producing the net radiated pattern?

RF
_____________

"Roy Lewallen" wrote:

A "non-radiating" feedline is one on which there is no net current
(i.e., no common mode current). In the case of coax, this translates to
zero current on the outside of the shield; for twinlead feedlines, it
means that the currents in the two conductors are exactly equal in
magnitude and opposite in direction.


A transmission line placed symmetrically with respect to a dipole
won't have any current induced in it, although current can be conducted
via a direct connection.


The amount of common mode current flowing in a transmission
line can be reduced by introducing an impedance to the common
mode current. It's desirable to do this without disturbing the differential
mode transmission line operation. That's the function of a balun.




Cecil Moore June 11th 04 09:48 PM

Richard Fry wrote:
A balun can reduce common mode feedline currents due to the power supplied
to the line by the transmitter, but if the feedline is immersed in an
asymmetric radiated field, how does the balun reduce/remove the resulting,
unpredictable differential current on the feedline, and its contribution
toward producing the net radiated pattern?


It simply provides an impedance to the common-mode currents. Whether
that impedance is high enough to be effective depends upon the system
parameters and configuration.
--
73, Cecil http://www.qsl.net/w5dxp



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Roy Lewallen June 11th 04 10:04 PM

The radiated field in which a feedline is immersed produces a common
mode, not differential, current on the feedline(*). The balun creates a
high impedance to the flow of common mode current. The result is that
much less common mode current is induced than would be the case if the
balun were absent. AM broadcasters put insulators periodically in tower
guy wires. Baluns have the same effect, although they're of course not
as perfect as the fully open circuit created by the insulator.

I'd also like to add that the induced current isn't unpredictable, as
you stated. It has to follow rules like all other physical phenomena, so
it's entirely predictable. I have to qualify this, though, by noting
that in many or most amateur installations, the path from the antenna
along the outside of the feedline to the rig and from there to the Earth
is often not well known. And precise predictions of feedline current
can't be made without knowing this path.

This effect is easily observed in models, as well as being
experimentally verifiable with a small amount of effort. For example,
make a simple wire Yagi with wire elements. Slip a few ferrite cores
over one of the elements and see what happens to the pattern. What
you've done is to reduce the current in the parasitic element, which is
immersed in the field from the driven and other elements, thereby
reducing its contribution to the total field. Cutting the element
(analogous to the broadcasters' insertion of an insulator) has the same
effect, although it'll be even more profound than the high but finite
impedance of the cores. Quanitative measurements aren't hard to make,
either. You can find details of current measurement devices in Chapter 8
of the ARRL Antenna book and other references. When placed over a coax
feedline, or over both conductors of a twinlead feedline, they'll
measure the common mode current.

(*) I'm assuming here that we're dealing either with coax, or with
twinlead whose wire spacing is small in terms of wavelength and whose
spacing from the antenna is large compared to the wire spacing. If you
put twinlead in a field such that the field seen by one conductor is
significantly different than the field seen by the other, you will get
an induced differential, as well as common mode current. This won't
happen with coax. Unlike common mode current, an induced differential
current will affect the properties of the line as a transmission line
(that is, change its apparent Z0 and velocity factor). But this would be
an unusual condition in an amateur installation, and I'm not considering
it here.

Roy Lewallen, W7EL

Richard Fry wrote:
A balun can reduce common mode feedline currents due to the power supplied
to the line by the transmitter, but if the feedline is immersed in an
asymmetric radiated field, how does the balun reduce/remove the resulting,
unpredictable differential current on the feedline, and its contribution
toward producing the net radiated pattern?

RF
_____________

"Roy Lewallen" wrote:

A "non-radiating" feedline is one on which there is no net current
(i.e., no common mode current). In the case of coax, this translates to
zero current on the outside of the shield; for twinlead feedlines, it
means that the currents in the two conductors are exactly equal in
magnitude and opposite in direction.



A transmission line placed symmetrically with respect to a dipole
won't have any current induced in it, although current can be conducted
via a direct connection.



The amount of common mode current flowing in a transmission
line can be reduced by introducing an impedance to the common
mode current. It's desirable to do this without disturbing the differential
mode transmission line operation. That's the function of a balun.





* June 11th 04 10:38 PM

Yes, it distorts the pattern, radiating or not.
How much depends upon the situation,
frequencies, spacing, size of feedline.
It is a conductive surface so it will distort pattern.
Side mounted on a tower changes pattern quite a lot
depending upon spacing from the tower, you can tune
the pattern that way. dB Products used to have a good
Catalogue that showed this.
I would not expect much pattern distortion from a feedline
very small, but would from a tower.



"Richard Fry" wrote in message
...
Post below from May 20, 2004

Wouldn't a "non-radiating" feedline in the field of a radiator also

distort
the patterns of that radiator? Any conductor can do that, even if it is

not
a feedline. NEC-2 models of FM broadcast transmit elements (and test

range
patterns) show this clearly.

Paper 6 at http://rfry.org shows the free space patterns that the element
arms of a rototiller FM broadcast transmit antenna develop if they could

be
driven from internal power sources -- and then the effects of adding the
element stem, mounts, feedline, and some nearby tower structure. The
patterns can get very skewed, even though the only radiators getting power
via a metallic path from the tx are the element arms themselves.

RF
____________

"Roy Lewallen" wrote
With a typical ground plane antenna, the feedline can radiate
significantly, distorting the pattern. This effect could easily be
different for the different antennas. Modeling indicates that two baluns
are often needed to suppress the current on the outside of the feedline.
A model which includes the feedline might give some insights as to why
the antennas behave so differently.






Richard Fry June 11th 04 11:01 PM

As a discussion point, consider 1/2-wave parasitic radiators sometimes
positioned within a foot or two of FM broadcast transmit elements, to
"shape" their patterns. This is the common technique used in "sidemount"
antennas that must meet FCC requirements for directional FM broadcast
assignments.

A parasitic itself is suspended mechanically in space by a non-metallic
support. It has no direct connection to the transmitter, and no conductive
physical path to any part of the antenna, its feedline, mounts, or
supporting structure.

Such parasitics do affect the net radiation pattern(s) of the array.

Isn't a "non-radiating" feedline with a balun just an arbitrary length of
conductor, but now with a metallically conductive path to the driven
element(s), as well?

The feedline (and other metallic structures) adjacent to an FM broadcast
transmit antenna will affect the radiation patterns of the antenna even
though the measured match between the feedline and antenna input is
extremely good (even 1:1 SWR) -- in which case the line should have no
differential current to produce such an effect. What is the explanation for
that, please?

RF
______________

"Roy Lewallen" wrote in message
...
The radiated field in which a feedline is immersed produces a common
mode, not differential, current on the feedline(*). ETC




Roy Lewallen June 11th 04 11:39 PM

Richard Fry wrote:
As a discussion point, consider 1/2-wave parasitic radiators sometimes
positioned within a foot or two of FM broadcast transmit elements, to
"shape" their patterns. This is the common technique used in "sidemount"
antennas that must meet FCC requirements for directional FM broadcast
assignments.

A parasitic itself is suspended mechanically in space by a non-metallic
support. It has no direct connection to the transmitter, and no conductive
physical path to any part of the antenna, its feedline, mounts, or
supporting structure.

Such parasitics do affect the net radiation pattern(s) of the array.

Isn't a "non-radiating" feedline with a balun just an arbitrary length of
conductor, but now with a metallically conductive path to the driven
element(s), as well?


No. A "non-radiating" feedline is one which has no significant amount of
common mode current. This can be accomplished by making the feedline a
length such that the induced current is minimal; by inserting a balun or
baluns; and/or by placing the feedline symmetrically with respect to the
antenna. I thought I had explained this -- I don't seem to be
communicating well.

The feedline (and other metallic structures) adjacent to an FM broadcast
transmit antenna will affect the radiation patterns of the antenna even
though the measured match between the feedline and antenna input is
extremely good (even 1:1 SWR) -- in which case the line should have no
differential current to produce such an effect. What is the explanation for
that, please?


We've been down this path before, and you've shown that you won't accept
the fact that SWR has nothing to do with whether or not common mode
current exists on a feedline, and there's nothing I've been able to do
to convince you otherwise. You also either haven't read or won't believe
that it's common mode, not differential, current that causes a line to
radiate and thereby contribute to the overall pattern. But hopefully
other readers have learned from this exchange. Once the basic principles
are grasped, these phenomena lose their mystery, and they're no longer
"unpredictable", but readily measured, modeled, and understood.

Based on past experience, nothing I say will sway you from the way
you've chosen to interpret observed phenomena. And I believe I've done
enough explaining so that any other readers, who are open to learning
some fundamentals, can come away with a better understanding. So that's
enough for now.

Roy Lewallen, W7EL


RF
______________

"Roy Lewallen" wrote in message
...

The radiated field in which a feedline is immersed produces a common
mode, not differential, current on the feedline(*). ETC





Richard Fry June 12th 04 02:08 AM

Just curious, Roy. Have you used EZNEC to model an FM broadcast transmit
array, feedlines and adjacent tower -- as in the models in Paper 6 at
http://rfry.org ? If so, and your pattern results are appreciably different
than those, for those same scenarios -- I'd truly appreciate learning from
you the reason(s) you might pose for that. Maybe I'm doing it wrong.

I'll be glad to send you the intermediate results: radiators alone, complete
elements with feedlines, complete elements with feedlines and tower.

RF



Ian White, G3SEK June 12th 04 08:35 AM

Roy Lewallen wrote:
I'd also like to add that the induced current isn't unpredictable, as
you stated. It has to follow rules like all other physical phenomena,
so it's entirely predictable.


The key to reducing the unwanted feedline current is that knowledge that
"it has to follow rules". We can't change the rules, but we *can* change
the antenna/feedline configuration so that the rules will work in our
favor.

These are the well-known physical rules about the way that voltages and
currents distribute themselves on wires, for example:

* Antenna wires carry standing waves of voltage and current, and also so
do feedlines if they carry net (common-mode or surface) RF currents.

* A voltage maximum is located at a current minimum, and vice versa.

* Maxima and minima are a quarter-wavelength apart.

* Current goes to zero at the physical end of a wire; voltage goes to
maximum.

Whenever you change the antenna/feedline configuration, the rules will
then force the voltage and current to rearrange themselves into a new
configuration also. So how can we "play the rules" to reduce unwanted
feedline currents?

For the moment, let's talk about coax feedline and unwanted surface
currents, because it's easier to insert chokes and also easier to
understand the results.

The unwanted surface current on the feedline has two components:
* Conducted current, launched onto the feedline from the hard-wired
connection at the feedpoint
* Induced current, caused by the feedline being placed in an EM field.

Wherever you insert a feedline choke along the feedline (by winding the
coax into a coil, or using ferrite loading) then you are creating a high
impedance which *forces* a current minimum at that point. The rules will
then force the current distribution along the feedline to change, so
that it meet this new additional requirement.

A choke balun at the feedpoint is the single most effective change you
can make, because it almost completely prevents conducted currents from
being launched onto the feedline.

That leaves the induced currents to be dealt with. These are typically
less of a problem than the conducted current, but are very hard to kill.
It's rather like trying to squeeze the air out of a long inflated tube.
Squeeze in one place by forcing a current minimum, and a new current
maximum will pop up a quarter-wavelength away.

Your feedpoint choke has defined a current minimum at the top of the
feedline, but by squeezing there you have created an induced current
maximum a quarter-wavelength down the feedline. So place another choke
there too, and the rules will make it impossible for ay significant
currents to build up between those two chokes. By making the rules work
in your favor, you have effectively killed the feedline current between
the two chokes.

The current won't quite go to zero, and a current maximum will certainly
try to pop up somewhere else, if the rules allow... but it probably
won't be as large as before, and you can chase that one down too.

There are many other ways to look at the problem, but I've found this
viewpoint of "playing the rules" to be quite a helpful one. I hope it
chimes with some other people too.


--
73 from Ian G3SEK 'In Practice' columnist for RadCom (RSGB)
http://www.ifwtech.co.uk/g3sek

Ian White, G3SEK June 12th 04 08:49 AM

Roy Lewallen wrote:
The feedline (and other metallic structures) adjacent to an FM broadcast
transmit antenna will affect the radiation patterns of the antenna even
though the measured match between the feedline and antenna input is
extremely good (even 1:1 SWR) -- in which case the line should have no
differential current to produce such an effect. What is the explanation for
that, please?


We've been down this path before, and you've shown that you won't
accept the fact that SWR has nothing to do with whether or not common
mode current exists on a feedline, and there's nothing I've been able
to do to convince you otherwise. You also either haven't read or won't
believe that it's common mode, not differential, current that causes a
line to radiate and thereby contribute to the overall pattern.


I agree with Roy that SWR itself is not the *cause* of radiating
feedlines.

However, if the feedline is allowed to carry currents and radiate, it
effectively becomes part of a new and different antenna configuration.
That new configuration will have a different feedpoint impedance, so the
SWR will change.

But the SWR didn't cause the feedline current and radiation; in fact it
was exactly the opposite.

Also, Richard is assuming that unwanted feedline currents will always
change the SWR for the worse. That's often true, but it doesn't have to
be - sometimes the SWR gets worse when the feedline current is choked
off.


--
73 from Ian G3SEK 'In Practice' columnist for RadCom (RSGB)
http://www.ifwtech.co.uk/g3sek

Dr. Slick June 12th 04 11:49 AM

Roy Lewallen wrote in message ...

No. A "non-radiating" feedline is one which has no significant amount of
common mode current. This can be accomplished by making the feedline a
length such that the induced current is minimal; by inserting a balun or
baluns; and/or by placing the feedline symmetrically with respect to the
antenna. I thought I had explained this -- I don't seem to be
communicating well.



What's up Roy? Long time no see!

Ok, well, I'd like to discuss this a bit.

So for most of the dipole based antennas (including Yagis), you
can use 6 turns of 4" diameter coils in the coax, to make an inductive
loop that is supposed to prevent current from moving down the outer
braid (non-radiating).




We've been down this path before, and you've shown that you won't accept
the fact that SWR has nothing to do with whether or not common mode
current exists on a feedline, and there's nothing I've been able to do
to convince you otherwise. You also either haven't read or won't believe
that it's common mode, not differential, current that causes a line to
radiate and thereby contribute to the overall pattern. But hopefully
other readers have learned from this exchange. Once the basic principles
are grasped, these phenomena lose their mystery, and they're no longer
"unpredictable", but readily measured, modeled, and understood.


Ok, so I understand how the common-mode-rejection-ratio works with
an audio amplifier that has an XLR cable input: signals in phase
(common
mode) will cancel each other out when they reach the input transformer
(balun). And although the XLR cable is shielded, the two signal wires
are more like a twin-lead transmission line instead of like coaxial
cable.

So i'm not sure how to ask this, but coxial cable is obviously a
much different beast than twin lead, so the concept of common-mode
currents
radiating from the line is a bit strange because the outer braid
completely
encloses the inner radial. But this is weird because coaxial cable is
unbalanced already, while twin-lead (or in the case of the audio XLR,
shielded twin lead) is balanced.

This is a discussion he

http://lists.contesting.com/archives.../msg00484.html



Slick

Cecil Moore June 12th 04 01:52 PM

Dr. Slick wrote:
So for most of the dipole based antennas (including Yagis), you
can use 6 turns of 4" diameter coils in the coax, to make an inductive
loop that is supposed to prevent current from moving down the outer
braid (non-radiating).


6 turns is probably not enough inductance to do much choking on 160m
or 80m.

If the dipole is non-resonant, 6 turns of coax may have very little
effect on any HF frequency.
--
73, Cecil http://www.qsl.net/w5dxp



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Richard Clark June 12th 04 03:45 PM

On Fri, 11 Jun 2004 15:39:59 -0700, Roy Lewallen
wrote:

This can be accomplished by making the feedline a
length such that the induced current is minimal; by inserting a balun or
baluns; and/or by placing the feedline symmetrically with respect to the
antenna. I thought I had explained this -- I don't seem to be
communicating well.


Hi Roy, Richard,

Perhaps it is because of the naming convention vs. application.

The term more appropriate to the Topic is RF Choke rather than BalUn
(which performs the choking action by implication, and could easily
fail that implication if the incorrect BalUn design is chosen).
Further, as you have noted in past correspondence Roy, a second Choke
(not BalUn) is often required for these VHF/UHF applications to
completely isolate the line.

73's
Richard Clark, KB7QHC

Richard Clark June 12th 04 04:50 PM

On 12 Jun 2004 03:49:05 -0700, (Dr. Slick) wrote:

So for most of the dipole based antennas (including Yagis), you
can use 6 turns of 4" diameter coils in the coax, to make an inductive
loop that is supposed to prevent current from moving down the outer
braid (non-radiating).


Hi OM,

Loop has a loaded meaning here in this group, the appropriate term
would be R.F. Choke. What you describe is adequate for many
applications but needs to be confirmed in practice.

There are three (3) conductors implicit in any discussion of
Transverse vs. Common Mode. They are the two wires and ground (ground
being the conductor in the either the sense of a body of available
charge, or a literal wire). If you have absolutely no reference to a
third source of charge, then there is no issue of Common Mode.

The twin lead model in any real application (be it window line, twin
lead, or your AF cables) has some interaction with ubiquitous ground
and this gives rise to Common Modality issues. These models are
fairly obvious, what follows reveals how you have missed the
translation to coax:

So i'm not sure how to ask this, but coxial cable is obviously a
much different beast than twin lead, so the concept of common-mode
currents radiating from the line is a bit strange because the outer braid
completely encloses the inner radial. But this is weird because coaxial cable is
unbalanced already, while twin-lead (or in the case of the audio XLR,
shielded twin lead) is balanced.


The discussions in this group are often on shaky ground (pun intended)
by lacking discussion of ground. The discussions in this group are
often on that same tremulous substrate when the arguments run to
Kirchhoff, and tectonic when Superposition is given its fanfare.

The Kirchhoff/Superposition failures of discussion revolve around the
normal observation in the reciprocity of load as source. For the coax
model, the two conductors are bound just as tightly as any twin lead
or conductor pair. If we were to terminate the coax at a shielded
load, then the self shielding property of the coax would obviate any
discussion of Common Mode. Aside from leakage (if you choose to use
braided shield), it is totally absent. If you replaced the coax with
twin lead, Common Mode WOULD become an issue (an inverse of
expectations), but I will suspend that to return to the coax issue you
ask to resolve.

The coax terminates in real world loads that are not shielded and THIS
imbalances the system. A current is imparted to the load, and a
voltage is developed across it (Kirchhoff/Ohm). To any other system
component, this voltage is a source (Superposition) potential
(irrespective of where the "energy" comes from). This source, now
translated and extended to the feedpoint, sees the antenna, and it
sees the coax shield which has some linkage to ground. That is, the
exterior of the coax is NOT the same conductor as the interior of the
coax. The interior path is self shielded, the exterior is definitely
not. Superposition allows us to discard the interior wire of the
coax, and to simply view this coax as a third wire whose path is
described by the exterior of the shield.

This load-as-source (Superposition), then sees more than one path to
ground: one, through the load as we know it (typically the antenna);
and two, the coax shield's exterior path. Both offer paths for
current and this current is the Common Mode current - by definition,
as they are referenced to the Common (ground).

Where the load is balanced like a dipole (a seriously flawed
presumption, but usefully accepted for the purpose of argument); then
those current paths are equal, out of phase, cancel, and conform to
the Transverse Mode. However, this balanced load has a reference to
ground (this is where the flawed presumption arises and reveals how
the Common Mode originates). So does the exterior of the coax shield.
Some part of the balanced load is out of phase with the coax shield,
and with ground completing the circuit (as both elements share this
Common) then current flows - Common Mode current.

If you snub the coaxial exterior path (or Choke it); then you will
successfully reduce that Common Mode current. Examples of snubbing
mechanisms are bountifully described in this group.

Twin lead applications suffer from Common Mode for the same reasons
when the "balanced" load is in fact unbalanced (quite simple when the
literal, physical load, the antenna, fails to present equal relations
to ground). This is seen when you observe a dipole with one leg drawn
down at an angle (or up away from ground for that matter). The visual
imbalance is as telling as any method to confirm. If one end of a
dipole is supported in the clear, and the other end runs flat into a
wooded area, there is the obvious visual imbalance that will in some
way force Common Mode currents into the pristine twin lead
configuration. The failure mechanisms are manifold, so further
elaboration is unnecessary.

To stir the controversy, the standard FCC model for an AM service
antenna (ground mounted monopole) is possibly the single best, real
example of a balanced system. ;-)

73's
Richard Clark, KB7QHC

Dr. Slick June 12th 04 09:03 PM

Cecil Moore wrote in message ...
Dr. Slick wrote:
So for most of the dipole based antennas (including Yagis), you
can use 6 turns of 4" diameter coils in the coax, to make an inductive
loop that is supposed to prevent current from moving down the outer
braid (non-radiating).


6 turns is probably not enough inductance to do much choking on 160m
or 80m.

If the dipole is non-resonant, 6 turns of coax may have very little
effect on any HF frequency.



What's up Cecil?

ok, you may be right about HF, but for VHF (30-300 MHz), 6 turns
in the coax is enough.

So have you made an inductive coil in coax for HF? If so, how
many turns did you need, and what was the diameter of the turns?

I may need to do this for an AM station one day, but maybe not
because most AM antennas are some sort of end-fed random length
wire with a tuner, where the wire length is greater than 1/4 wavelength.
In other words, i haven't seen any dipole antennas for broadcast band
AM....it would be too long!


Slick

Cecil Moore June 12th 04 09:19 PM

Dr. Slick wrote:
So have you made an inductive coil in coax for HF? If so, how
many turns did you need, and what was the diameter of the turns?


I once made one out of a 2-liter pop bottle about 1/3 full
of turns of RG-8X. It worked pretty well on 40m, my favorite
band, but a thunderstorm destroyed it. I have no idea what
the choking impedance was.
--
73, Cecil http://www.qsl.net/w5dxp



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KC1DI June 12th 04 10:19 PM

On Sat, 12 Jun 2004 07:52:50 -0500, Cecil Moore
wrote:

Dr. Slick wrote:
So for most of the dipole based antennas (including Yagis), you
can use 6 turns of 4" diameter coils in the coax, to make an inductive
loop that is supposed to prevent current from moving down the outer
braid (non-radiating).


6 turns is probably not enough inductance to do much choking on 160m
or 80m.

If the dipole is non-resonant, 6 turns of coax may have very little
effect on any HF frequency.


It took 27 turn here to get decent choking on 80m. But it finally
worked 6" diamater selenoid wound.
73 Dave KC1DI

P.S. feeding a OFCD cut for 3.6 MHZ. Thru a 4 to 1 Balun.


Dr. Slick June 13th 04 10:51 PM

Richard Clark wrote in message . ..


(Large paragraphs of Nonsensical, pyseudo-technobable snipped)


The discussions in this group are often on shaky ground (pun intended)
by lacking discussion of ground. The discussions in this group are
often on that same tremulous substrate when the arguments run to
Kirchhoff, and tectonic when Superposition is given its fanfare.



It seems you are still spouting out words and concepts that you
really don't understand, eh? If things are on shaky ground here,
you certainly ain't helpin'!

This is a reminder that ANYONE can post anything they want here.


Slick
Slick

Richard Clark June 13th 04 11:04 PM

On 13 Jun 2004 14:51:20 -0700, (Dr. Slick) wrote:
This is a reminder that ANYONE can post anything they want here.

Self-fulfilling prophesy?

Slick
Slick

redundant or hyperbolic comment?

Hi OM,

Again, you haven't the talent to attack on style nor bandwidth to
challenge technical content. If you responded to the issue you are
having difficulty with, then that would be another matter.

Try again. ;-)

73's
Richard Clark, KB7QHC

Reg Edwards June 14th 04 01:42 AM


Perhaps I might be of assistance by providing some orders of magnitude.

A 1/2-wave stub line, 1 metre (39.37 inches) long constructed of a pair of
polished copper tubes, each 1/2-inch in diameter, centers spaced 3 inches
apart, at 150 MHz (not very far from 2 meters) has the following
characteristics -

Zo = 299.8 ohms.
Attenuation = 0.0024 dB.
As a tuned circuit, Resonant Q = 5800.

When short-circuited -
Parallel input components of Zin -
Rsc = 0.08 ohms,
Xsc = -j*582 ohms.

When open circuited -
Series input components of Zin -
Roc = 1.11 megohms,
Xoc = j*38.6 ohms.

These and many other interesting values can be very accurately and rapidly
calculated, from 20 Hz to 1 GHz, by using program RJELINE2 available, free
issue, from website below.

Contributors to this newsgroup, who by no means are lacking in intelligence,
may then be able to get their feet on the ground.
-----
.................................................. ..........
Regards from Reg, G4FGQ
For Free Radio Design Software go to
http://www.btinternet.com/~g4fgq.regp
.................................................. ..........



MikeN June 15th 04 02:40 AM

On Sat, 12 Jun 2004 08:35:42 +0100, "Ian White, G3SEK"
wrote:

Roy Lewallen wrote:
I'd also like to add that the induced current isn't unpredictable, as
you stated. It has to follow rules like all other physical phenomena,
so it's entirely predictable.


Remainder deleted


Three questions emerge from my foggy brain wrt to a current project.

1. What sort of choke loading on a feed line would be most
effective at 70 cm, ferrite or coil wound from coax.

2. Could ferrite loading at a feed point take the place of say a
1/4 wave sleeve balun matching the unbalanced coax feed to a
centre-fed dipole element.

3. What grade of ferrite bead would best be useful at 70cm.

Thanks in advance.

MikeN ZL1BNB

Roy Lewallen June 15th 04 04:29 AM

MikeN wrote:

Three questions emerge from my foggy brain wrt to a current project.

1. What sort of choke loading on a feed line would be most
effective at 70 cm, ferrite or coil wound from coax.


Probably equally effective, although it might be tricky to get a coax
coil to resonate at 70 cm, while a ferrite core choke, which is
inherently broadband, would be easy.

2. Could ferrite loading at a feed point take the place of say a
1/4 wave sleeve balun matching the unbalanced coax feed to a
centre-fed dipole element.


Yes. A properly constructed sleeve balun can be made to have higher
impedance, but in the application you describe, a ferrite core choke
would be perfectly adequate.

3. What grade of ferrite bead would best be useful at 70cm.


I'd probably use type 43. That's a Fair-Rite designation, but ferrites
from other vendors with initial permeability of 700-800 or so would work
equally well. Cores from that material are readily available in a wide
variety of shapes and sizes. Some of the 60 series ferrites would also
probably be adequate at that frequency.

I suggest you visit the Fair-Rite website and take a look at the
impedances of various cores at the frequency of interest, and choose
ones that get you the impedance you need. (Unless you're running a lot
of power, you don't need to worry about whether the impedance is
resistive or reactive -- just look at its magnitude.) You can place
cores on the outside of the coax and get an imedance that's the product
of the number of cores and the impedance of one core. Or you can wind
the coax in multiple turns on a single core and get N^2 times the single
turn impedance, where N is the number of turns. 500 - 1000 ohms or so of
impedance is adequate for most applications. If you have an antenna
analyzer that operates at that frequency, you can measure it. Otherwise,
just go by the manufacturer's stated value of impedance at the frequency
of interest.

Roy Lewallen, W7EL


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