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-   -   Shorted 1/4 wave stub ? (https://www.radiobanter.com/antenna/1882-shorted-1-4-wave-stub.html)

Cecil Moore June 11th 04 09:52 PM

Dave Shrader wrote:
So, are you pursuing Physics or Applications type knowledge?


And apparently, never the twain shall meet. :-)



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Henry Kolesnik June 11th 04 10:25 PM

What happens if the twisted short is grounded as in lightning protection?
Is there any succinct difference?

--
73
Hank WD5JFR

"Cecil Moore" wrote in message
...
Reg Edwards wrote:

By how much does the length of the short-circuiting bar at the end of

the
1/4-wave stub affect its resonant length?


I just twist the ends together. I don't use a bar.

What open-circuit resonant frequency does the stub change to when the

short
circuiting bar is removed?


Same resonant frequency - virtual impedance at the input is reversed.
--
73, Cecil http://www.qsl.net/w5dxp



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Dave Shrader June 12th 04 10:29 PM

Dave wrote:
you can look at it various ways.


As I mentioned above; engineers, technicians, wave mechanics,
physicists, experimenters, etc., ALL live on this list grin. Mea
Culpa, I'm a retired engineer.

Just remember, stubs WORK very well. Thank the owner of your local
repeater for tuning the stubs [AKA CAVITIES] to reduce the desense below
receiver response levels, typically -120 dB or more attenuation.


1. the wave traveling wave analysis... the harmonic goes down the stub,
reflects back, and when it gets back to the transmission line it is 180
degress out of phase with the next cycle so it cancels it at the junction...
therefore there is no harmonic to propagate down the line past the junction.
this of course will raise the hackles of the anti-reflectionists who will
then say there is also no harmonic left to propagate down the stub which
means there is a virtual short at the junction, but no way to generate it
since nothing can be there to go down the stub.

2. the power analysis. power goes in, power comes out, it all reflects back
and forth until the energy becomes infinite and the amp blows up... but of
course energy is conserved and momentum must go somewhere so the stub
probably walks across the table with each wave reflection.

3. the sinusoidal steady state analysis. this takes the stub and transforms
the shorted impedance at the far end back to the junction and then does all
calculations as if the real short existed at the junction.... this will of
course annoy the reflectionists who will point out in never ending detail
how you can't explain tv ghosts, radar, or other transient phenomena this
way... of course by assuming the sinusoidal steady state at the start you
exclude those systems from this type of analysis, but that won't stop the
protests.

4. the s analysis... who know what this will say except cecil who will find
some way to steer the discussion over to it.

5. the optical layer analysis... see above.

"Henry Kolesnik" wrote in message
...

I know they work! One of my reasons for asking the question is I've not
found any mention in the literature of where the
"attenuation/rejection/reflection/filter residue" goes.

--
73
Hank WD5JFR
"Dave" wrote in message
...

the harmonic is 'attenuated' in that the magnitude of it is reduced when


the

stub is in line. i look at it like you could replace the stub with a


lumped

filter at the same point so the term attenuation makes more sense than
reflections or rejections... i don't really care where the harmonic


goes,

i

want to know how much it is attenuated by so i can compare with other


types

of filters.

"Henry Kolesnik" wrote in message
.com...

Dave

Nice site, I like the "white paper" approach as I prefer the info


without

the glitter. I've only read a few items and I
quote: "This is a plot of the attenuation provided by the stub. You


can

see

that it provides about 32db of attenuation at 28.25Mhz. " I've


noticed

that

the literature I've purused indicates that stubs either attenuate or

reject.

None say reflect! I don't want to get into a discussion of word

definitions

becasue reflect and feject are close but attenuate is not in the same

class.

Comments...

--
73
Hank WD5JFR

"Dave" wrote in message
...

"Henry Kolesnik" wrote in message
y.com...

I know that a shorted 1/4 wave stub exhibits a very high


impedance.

But

for the 2nd harmonic it's a 1/2 wave stub and exhibits a very low

impedance

or a short. There are claims that this can be used to filter the


even

harmonics. Shorts can't diisipate power and must reflect, so how

does

a

stub work?

stubs work very nicely. you can get practical stub information at


my

web

site, including how to build a 40m to 15m 3rd harmonic stub filter:
http://www.k1ttt.net/technote/techref.html#filters

as you may have noticed by now you have kicked the proverbial


hornets

nest.

reflections are a touchy word in this group, usually attracting the

endless

argument that travels from thread to thread. in time this will

deteriorate

into name calling and endless argument over reflections,


interference,

virtual impedances, and a few other topics.











Richard Clark June 12th 04 11:05 PM

On Fri, 11 Jun 2004 18:32:14 GMT, "Henry Kolesnik"
wrote:
What if the source doesn't or can't dissipate?


Hi Hank,

Simple enough to find out. Disconnect the output of your transmitter.
Set the drive level of your transmitter for full power. Defeat the
ALC. Key down. By the clock or watch, take notes at 1 minute
intervals for, say, 10 minutes. Prepare notes into report. Submit
report here. Total time to perform: 30 seconds - 30 minutes depending
mostly on access to the ALC defeat.

This answers all equivocations about does/doesn't; will/won't;
might/mightn't; could/couldn't; or can/can't. Think about it, you
have probably spent more time than that writing to and reading from
this thread to no certain conclusion.

73's
Richard Clark, KB7QHC

Dave Shrader June 12th 04 11:58 PM

Cecil Moore wrote:

SNIP

Heh, heh, you're on your own for that discussion. I personally
believe it is possible for reflected energy to wind up decreasing
the power consumption from the DC source that is supplying the finals,
which winds up decreasing the load on the 60 Hz power grid, which
decreases the oil required from the Middle East, which tends to
decrease the possibility of world war, which bodes well for the human
race, but that is another thread for another time.
--
73, Cecil http://www.qsl.net/w5dxp


Good engineering CAN solve the world's problems!!!

Just use enough 1/4 wavelength stubs and we can totally eliminate the #1
or #2 cause of international tension!!

Now, the Oil exporting states will face economic ruin! We will have to
give them foreign aid!! Damn ... taxes will have to go up!! That means
we have to elect a Demo Krapp as president.

Cecil, I didn't know you were campaigning for what's his name!!

I better be careful or my tongue may slip out of my cheek.


Al June 13th 04 04:22 AM

Sometimes, it's useful to think about problems such as this in terms of
analogous systems that behave in similar ways.

For example, imagine a gasoline-powered engine driving a water pump though a
friction belt and pulley. The pump is attempting to pump water into a short
plugged pipe (shorted transmission line). After the first couple of seconds
the reflected water from the plugged end creates a back pressure on the
pump, a situation in which the pump is then not capable of delivering
additional water to that which is stored in the pipe. Now, a number of
things can occur, short of mechanical failure of some part of the system:

1) the belt between the motor and pump can start to slip, dissipating the
energy generated by the motor as heat lost to friction in the belt and
pulley

2) the motor can slow or cease to function, incapable of working against the
increased torque (impedance) created by the belt that has been constrained
by the pump that can't pump water into the plugged pipe.

In case 1), the power is being generated by the motor, but it is not being
delivered to the load. It is being dissipated (converted to heat) `in
between.
In case 2), the power simply cannot be created. The motor can't work against
such a load. The power is not being dissipated anywhere -- it's simply not
being generated. As Cecil has suggested, in this case, the engine stops,
which stops using gasoline, which reduces the demand on the Middle East oil
supply, which lowers prices, which .....

Case 2) is not one in which reflections "cancel" the energy being generated,
although it can be thought of that way. Energy can't be "canceled" ( a
fundamental law). If a generator isn't delivering energy to a load, it's
because the energy either doesn't exist (isn't being generated), or it's
being rerouted, stored, or being converted to another form.

Although this analogy could be complicated by making it a pumping system
that generates sinusoidal water pressure waves with wavelength-related pipe
lengths, it doesn't need to be for it to work.

Al WA4GKQ


"Cecil Moore" wrote in message
...
Henry Kolesnik wrote:
What if the source doesn't or can't dissipate?


Heh, heh, you're on your own for that discussion. I personally
believe it is possible for reflected energy to wind up decreasing
the power consumption from the DC source that is supplying the finals,
which winds up decreasing the load on the 60 Hz power grid, which
decreases the oil required from the Middle East, which tends to
decrease the possibility of world war, which bodes well for the human
race, but that is another thread for another time.
--
73, Cecil http://www.qsl.net/w5dxp



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Henry Kolesnik June 13th 04 04:47 PM

Better specify the kind of pump because a centrifugal will have a different
outcome versus a positive displacment!

--
73
Hank WD5JFR
"Al" wrote in message
...
Sometimes, it's useful to think about problems such as this in terms of
analogous systems that behave in similar ways.

For example, imagine a gasoline-powered engine driving a water pump though

a
friction belt and pulley. The pump is attempting to pump water into a

short
plugged pipe (shorted transmission line). After the first couple of

seconds
the reflected water from the plugged end creates a back pressure on the
pump, a situation in which the pump is then not capable of delivering
additional water to that which is stored in the pipe. Now, a number of
things can occur, short of mechanical failure of some part of the system:

1) the belt between the motor and pump can start to slip, dissipating the
energy generated by the motor as heat lost to friction in the belt and
pulley

2) the motor can slow or cease to function, incapable of working against

the
increased torque (impedance) created by the belt that has been constrained
by the pump that can't pump water into the plugged pipe.

In case 1), the power is being generated by the motor, but it is not being
delivered to the load. It is being dissipated (converted to heat) `in
between.
In case 2), the power simply cannot be created. The motor can't work

against
such a load. The power is not being dissipated anywhere -- it's simply not
being generated. As Cecil has suggested, in this case, the engine stops,
which stops using gasoline, which reduces the demand on the Middle East

oil
supply, which lowers prices, which .....

Case 2) is not one in which reflections "cancel" the energy being

generated,
although it can be thought of that way. Energy can't be "canceled" ( a
fundamental law). If a generator isn't delivering energy to a load, it's
because the energy either doesn't exist (isn't being generated), or it's
being rerouted, stored, or being converted to another form.

Although this analogy could be complicated by making it a pumping system
that generates sinusoidal water pressure waves with wavelength-related

pipe
lengths, it doesn't need to be for it to work.

Al WA4GKQ


"Cecil Moore" wrote in message
...
Henry Kolesnik wrote:
What if the source doesn't or can't dissipate?


Heh, heh, you're on your own for that discussion. I personally
believe it is possible for reflected energy to wind up decreasing
the power consumption from the DC source that is supplying the finals,
which winds up decreasing the load on the 60 Hz power grid, which
decreases the oil required from the Middle East, which tends to
decrease the possibility of world war, which bodes well for the human
race, but that is another thread for another time.
--
73, Cecil http://www.qsl.net/w5dxp



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Henry Kolesnik June 13th 04 04:49 PM

This place is where one can just about learn anything or nothing or learn
incorreclty. AKA the politics of reflections.

--
73
Hank WD5JFR
"Richard Clark" wrote in message
...
On Fri, 11 Jun 2004 18:32:14 GMT, "Henry Kolesnik"
wrote:
What if the source doesn't or can't dissipate?


Hi Hank,

Simple enough to find out. Disconnect the output of your transmitter.
Set the drive level of your transmitter for full power. Defeat the
ALC. Key down. By the clock or watch, take notes at 1 minute
intervals for, say, 10 minutes. Prepare notes into report. Submit
report here. Total time to perform: 30 seconds - 30 minutes depending
mostly on access to the ALC defeat.

This answers all equivocations about does/doesn't; will/won't;
might/mightn't; could/couldn't; or can/can't. Think about it, you
have probably spent more time than that writing to and reading from
this thread to no certain conclusion.

73's
Richard Clark, KB7QHC




Dave Shrader June 13th 04 07:54 PM

Is there any objective reality when it comes to reflections? How do we
really know?

Henry Kolesnik wrote:

This place is where one can just about learn anything or nothing or learn
incorreclty. AKA the politics of reflections.



Henry Kolesnik June 13th 04 08:21 PM

Well perhaps I should reword my comment. It seems like many responders are
getting into the politics of reflections, some into the theory but I believe
it's a science and should be explainable. Theories are used to explain what
goes on inside a black box that we can't open, just an input and output.
But a shorted 1/4 wave stub is about as far as you can get from a black
box.. I'm curious!
There are no stupid questions, just stupid people asking and that's me.

--
73
Hank WD5JFR
"Dave Shrader" wrote in message
news:Mp1zc.42427$HG.38082@attbi_s53...
Is there any objective reality when it comes to reflections? How do we
really know?

Henry Kolesnik wrote:

This place is where one can just about learn anything or nothing or

learn
incorreclty. AKA the politics of reflections.





Richard Clark June 13th 04 08:29 PM

On Sun, 13 Jun 2004 18:54:36 GMT, Dave Shrader
wrote:
Is there any objective reality when it comes to reflections? How do we
really know?


Hi Dave,

I offered a very simple test. There is the path of an objective
result, or the path of a subjective and ponderous appeal.

You do have a rig, do you not? You could perform the several steps to
come to a conclusion I presume - otherwise disabuse me of this talent
I inferred in your behalf and state which political party you are
affiliated with.

73's
Richard Clark, KB7QHC

Cecil Moore June 13th 04 08:47 PM

Dave Shrader wrote:
Is there any objective reality when it comes to reflections? How do we
really know?


Use a TDR. Observe TV ghosting. The reflection model is perfectly
valid and consistent and the outcomes using the reflection model
are the same as any other valid consistent model. An S-parameter
analysis uses reflection/transmission coefficients, i.e. the wave
reflection model. If an S-parameter analysis is not valid, a whole
@#$%-load of electronics should not be functioning as they do.

I'm not entirely certain, but I believe the H-parameter analysis,
the Y-parameter analysis, and the Z-parameter analysis all use
the reflection model and are valid for impedance discontinuities
in transmission lines.
--
73, Cecil http://www.qsl.net/w5dxp



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Richard Clark June 13th 04 08:49 PM

Originally you asked:
so how does a stub work?


On Sun, 13 Jun 2004 19:21:19 GMT, "Henry Kolesnik"
wrote:

Well perhaps I should reword my comment.

snip complaint of politics
But a shorted 1/4 wave stub is about as far as you can get from a black
box.. I'm curious!


Hi Hank,

Seems like several many have offered the simple mechanics to satisfy
the question.

Would you like to comment why they did not? If you find the
reflection based argument tedious (and it can be that in spades); then
perhaps you should offer an outline of the terms to be employed or the
constraints of the stub's application to reduce shot-gun answers that
bloat the thread.

73's
Richard Clark, KB7QHC

Cecil Moore June 13th 04 08:54 PM

Henry Kolesnik wrote:

Well perhaps I should reword my comment. It seems like many responders are
getting into the politics of reflections, some into the theory but I believe
it's a science and should be explainable. Theories are used to explain what
goes on inside a black box that we can't open, just an input and output.
But a shorted 1/4 wave stub is about as far as you can get from a black
box.. I'm curious!
There are no stupid questions, just stupid people asking and that's me.


The solid-state political creed seeks to discredit reflections by using
only the solid-state shortcut physics. These shortcuts certainly work,
but they do not dictate reality. Man, not Mother Nature, takes those
shortcuts. Witness the inability of anyone to present an example of
the existence of standing-waves in a single source, single feedline,
single mismatched load system, without the existence of a forward-
traveling wave and a rearward-traveling (reflected) wave.

The same solid-state political creed dictates the definition of source
power. It says that if reflected power is taken in the source, then
it was never generated in the first place. Never mind that energy can
be proven to have made a round-trip to the load and back to the source.
--
73, Cecil http://www.qsl.net/w5dxp



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Cecil Moore June 13th 04 08:57 PM

Richard Clark wrote:

Dave Shrader wrote:
Is there any objective reality when it comes to reflections? How do we
really know?


I offered a very simple test.


First, you must prove that you are a member of objective reality.
That's a very difficult assignment, given most of your postings. :-)
--
73, Cecil http://www.qsl.net/w5dxp



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Richard Clark June 13th 04 09:06 PM

On Sun, 13 Jun 2004 14:57:11 -0500, Cecil Moore
wrote:
I offered a very simple test.

First, you must prove that you are a member of objective reality.

too simple to perform, hmm?

Dave Shrader June 13th 04 09:53 PM

Richard Clark wrote:

SNIP

Hi Dave,

I offered a very simple test. There is the path of an objective
result, or the path of a subjective and ponderous appeal.

You do have a rig, do you not? You could perform the several steps to
come to a conclusion I presume - otherwise disabuse me of this talent
I inferred in your behalf and state which political party you are
affiliated with.

73's
Richard Clark, KB7QHC


Richard, I'm a retired EE and have used stubs extensively in USAF
Missile systems C-band and S-band design. They work, they get warm, they
increase the insertion loss in the transmission line system, they work,
they work, ...

We use the word 'THEORY' too loosely in ham discussions. Theory is the
state of experimental verification between Hypothesis and Law. Many
times we use the word 'Theory' when we should say that
Physics/Mathematics explain the observation as follows: etc.

In a shorted 1/4 wavelength transmission line 'stub' we have a current
maximum at the physical short circuit. We have a high impedance 1/4
wavelength from the physical short circuit. The voltage and current have
a sinusoidal relationship along the length of the 'stub'. There is a
forward and reflected wave within the 'stub'.

There are several loss components within the 'stub' including I^2*R and
V^2/Rl [Capacitive dielectric losses] and 1/2L*I^2 [Leakage Inductance
losses]. Therefore the presence of a stub increase the insertion loss in
the transmission line sub-system; conversely, the removal of the stub
reduces the insertion loss in the transmission line sub-system.

In EM Physics, circa 1958-59, the equations of state for the stub
included both a transient response and a steady state response. I have
not solved these equations in more than 20 years [I probably forgot how
to solve them in any event! ]

With all this said and done I find it interesting to follow the
discussions and learn many things, some of which are correct grin.


Dave Shrader June 13th 04 10:06 PM

In the absence of an observer there is no objective reality.

In the absence of an observer any reality, if it exists, is unknowable.

I observe, therefore ...

+ + +

Cecil Moore wrote:


First, you must prove that you are a member of objective reality.
That's a very difficult assignment, given most of your postings. :-)
--
73, Cecil http://www.qsl.net/w5dxp




Reg Edwards June 13th 04 11:43 PM

With all this said and done I find it interesting to follow the
discussions and learn many things, some of which are correct grin.

=================================

How do you know you are learning anything?



Cecil Moore June 14th 04 01:26 AM

Dave Shrader wrote:
In EM Physics, circa 1958-59, the equations of state for the stub
included both a transient response and a steady state response.


Hey Dave, looks like we both studied the same physics. But did you know
that Mother Nature changed her mind during the last 50 years? :-)
--
73, Cecil http://www.qsl.net/w5dxp



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Tdonaly June 14th 04 03:34 PM

Cecil wrote,

I'm not entirely certain, but I believe the H-parameter analysis,
the Y-parameter analysis, and the Z-parameter analysis all use
the reflection model and are valid for impedance discontinuities
in transmission lines.
--
73, Cecil http://www.qsl.net/w5dxp



Those are all examples of two port parameters, good for your basic linear,
time invariant system. (While you're at it, don't forget the
transmission parameters, Cecil.) They'll work with any old lumped
or distributed system as long as it's linear, has two ports, and is
time invariant.

You can't really use S-parameters to prove reflections exist because
S-parameter theory assumes reflections exist even when they don't, as in the
case of
transistor characterization - much like calculating the VSWR in a
zero length transmission line. They're good for analysis, though, as long
as you don't get carried away and look on them as proving something about
God, the Universe and Everything.
73,
Tom Donaly, KA6RUH



Cecil Moore June 14th 04 07:55 PM

Tdonaly wrote:
You can't really use S-parameters to prove reflections exist because
S-parameter theory assumes reflections exist even when they don't, ...


On the contrary, if one assumes same-cycle reflections, the reflection
model works perfectly. Why wouldn't a 50 ohm source looking into a 100
ohm resistor suffer an immediate reflection (energy rejection)? :-)
--
73, Cecil http://www.qsl.net/w5dxp



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Tdonaly June 14th 04 10:28 PM

Cecil wrote,
Message-id:

Tdonaly wrote:
You can't really use S-parameters to prove reflections exist because
S-parameter theory assumes reflections exist even when they don't, ...


On the contrary, if one assumes same-cycle reflections, the reflection
model works perfectly. Why wouldn't a 50 ohm source looking into a 100
ohm resistor suffer an immediate reflection (energy rejection)? :-)
--
73, Cecil http://www.qsl.net/w5dxp



Why wouldn't it, indeed.
73,
Tom Donaly, KA6RUH



Dave June 14th 04 10:39 PM

"Tdonaly" wrote in message
...
Cecil wrote,
Message-id:

Tdonaly wrote:
You can't really use S-parameters to prove reflections exist because
S-parameter theory assumes reflections exist even when they don't,

....

On the contrary, if one assumes same-cycle reflections, the reflection
model works perfectly. Why wouldn't a 50 ohm source looking into a 100
ohm resistor suffer an immediate reflection (energy rejection)? :-)
--
73, Cecil http://www.qsl.net/w5dxp



Why wouldn't it, indeed.
73,
Tom Donaly, KA6RUH



if there are no components that introduce a time delay it would. so no
transmission lines allowed... hence no reflections. and you are back to a
simple lumped resistor problem.




Cecil Moore June 15th 04 04:32 AM

Dave wrote:
"Tdonaly" wrote:

Cecil wrote,
On the contrary, if one assumes same-cycle reflections, the reflection
model works perfectly. Why wouldn't a 50 ohm source looking into a 100
ohm resistor suffer an immediate reflection (energy rejection)? :-)


Why wouldn't it, indeed.


if there are no components that introduce a time delay it would.


All real-world components introduce a time delay.

so no
transmission lines allowed... hence no reflections. and you are back to a
simple lumped resistor problem.


RF energy travels at the speed of light. For the length of time it
takes for the energy to reach the resistor and reflect back to the
source, the source sees 50 ohms. That length of time is not zero.
--
73, Cecil http://www.qsl.net/w5dxp



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Tdonaly June 15th 04 06:14 AM


Dave wrote,


if there are no components that introduce a time delay it would. so no
transmission lines allowed... hence no reflections. and you are back to a
simple lumped resistor problem.



Maybe, but don't tell that to the analytical types. Zero length transmission
lines are part of the stock in trade of some people who find the concept
useful.
73,
Tom Donaly, KA6RUH



Tdonaly June 15th 04 06:40 AM

Cecil wrote,

RF energy travels at the speed of light. For the length of time it
takes for the energy to reach the resistor and reflect back to the
source, the source sees 50 ohms. That length of time is not zero.
--
73, Cecil http://www.qsl.net/w5dxp



Even though the length of time is not zero, it's close enough
so that the theorems of network analysis work (at least
at the lower frequencies). Of course, if you want to do a reflection analysis
on a
couple of resistors, each of which is only a minute fraction of
a wavelength long, well, it's a free country. S-parameters assume
reflections and such, and are very useful to the people who use them,
but, as an intellectual tool, it doesn't matter whether there are any real
reflections or not as long as the answers come out right. They
don't really prove reflections in and of themselves, anyway, since it's hard to

prove something based on the assumption that it's true. (I assume it, therefore

it's true.)
73,
Tom Donaly, KA6RUH



Cecil Moore June 15th 04 12:15 PM

Tdonaly wrote:
Dave wrote,
if there are no components that introduce a time delay it would. so no
transmission lines allowed... hence no reflections. and you are back to a
simple lumped resistor problem.

Maybe, but don't tell that to the analytical types. Zero length transmission
lines are part of the stock in trade of some people who find the concept
useful.


At 3 GHz, one inch of wire is close to 1/4WL. :-)
12*984'/3000 = 3.936"
--
73, Cecil http://www.qsl.net/w5dxp



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Richard Clark June 15th 04 04:48 PM

On Tue, 15 Jun 2004 06:15:16 -0500, Cecil Moore
wrote:
At 3 GHz, one inch of wire is close to 1/4WL

At 3 GHz nobody uses wire.

Steve Nosko June 15th 04 08:00 PM


"Cecil Moore" wrote in message
...
Tdonaly wrote:
Dave wrote,
if there are no components that introduce a time delay it would. so no
transmission lines allowed... hence no reflections. and you are back to

a
simple lumped resistor problem.

Maybe, but don't tell that to the analytical types. Zero length

transmission
lines are part of the stock in trade of some people who find the concept
useful.


At 3 GHz, one inch of wire is close to 1/4WL. :-)
12*984'/3000 = 3.936"
--
73, Cecil http://www.qsl.net/w5dxp


Now I get it! (Cecil, that is) LOL

Just like the Civil Defense days... "This is a test. Had it been an actual
response, Cecil would have made an intelligent comment about the real
question". What a "tweeker", is Cecil. What a little devil. (:-)
I'm thinkn' it proves the old adage about the idle mind and a workshop....

73, Steve


P.S. Remember that sea of entropy we were supposed to drown in? Well, upon
closer examination, it turns out to be ignorance.

BTW... This is my comment on the general population, not any specifics
here...





Cecil Moore June 16th 04 03:10 AM

Richard Clark wrote:

Cecil Moore wrote:
At 3 GHz, one inch of wire is close to 1/4WL


At 3 GHz nobody uses wire.


The "why" of that statement proves my point.



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Richard Clark June 16th 04 04:09 AM

On Tue, 15 Jun 2004 21:10:54 -0500, Cecil Moore
wrote:
At 3 GHz, one inch of wire is close to 1/4WL

At 3 GHz nobody uses wire.

The "why" of that statement proves my point.

It is Tom's match point.

Cecil Moore June 16th 04 05:05 AM

Richard Clark wrote:
Cecil Moore wrote:

At 3 GHz, one inch of wire is close to 1/4WL

At 3 GHz nobody uses wire.


The "why" of that statement proves my point.


It is Tom's match point.


Doubt it. EM waves travel the same speed at 1 MHz or 3 GHZ.
If you get a reflection at 3 GHz, you certainly get a
reflection at 1 MHz. All the steady-state shortcuts in
the world won't change that fact of physics. What's sad
is you don't even realize it.
--
73, Cecil http://www.qsl.net/w5dxp



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Richard Clark June 16th 04 05:24 AM

On Tue, 15 Jun 2004 23:05:23 -0500, Cecil Moore
wrote:
don't even realize it

;-)

Richard Harrison June 16th 04 03:57 PM

Henry, WD5JFR wrote:
"Shorts can`t dissipate power, so how does a stub work?"

Henry also wrote:
"I know that a shorted 1/4 wave stub exhibits a very high impedance. But
for the 2nd harmonic it`s a 1/2 wave stub and exhibits a very low
impedance or a short."

Henry is correct.

Connect a resistance directly to a transmitter. How much energy is
absorbed by the resistance? Ohm`s law is the first approximation.
Current is directly proportional to the applied voltage if the
transmitter`s internal reistance is negligible.

The shorted 1/4-wave stub exhibits an open circuit at its mouth and
accepts only enough current to supply its losss which are none in the
perfect stub. So, it takes no power from the transmitter afer its
circulating current is etablished.
At 2X the 1/4-wave freqency, the stub is 1/2 wavelengh and does not
transform the short at one end to an open circuit at its other end.
Instead, the 1/2-wave directly presents the short circuit at its far
end.

How much curent can the transmitter supply to a short circuit? It
depends on the internal impedance of the transmitter.

"Transmission Lines, Antennas, and Wave Guides" by King, Mimno, and Wing
explains how "Even Harmonics" are suppressed by the 1/4-wave
short-circuited stub on page 29. The gist is that the stub is imperfect
and its resistance saps harmonic energy which is allowed into the stub
by its low impedance.

Best regards, Richard Harrison, KB5WZI


Cecil Moore June 16th 04 05:04 PM

Richard Harrison wrote:
The shorted 1/4-wave stub exhibits an open circuit at its mouth and
accepts only enough current to supply its losss which are none in the
perfect stub.


Richard, I think you would be surprised if you measured the RF current
through the short at the shorted end. It will be the in-phase sum of
the forward current and reflected current and is quite high. I once
melted the insulation at the end of a shorted 1/4WL piece of RG8X.
The heat came from high I^2*R losses at the short.

The SWR inside a perfect stub is infinite.
--
73, Cecil http://www.qsl.net/w5dxp



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Richard Harrison June 16th 04 08:03 PM

Cecil, W5DXP wrote:
"Richard, I think you would be surprised if ypu measured RF current
through the short at the shorted end."

I expect high circulating current but without loss not much current is
required of the power source.

In his 1955 edition on page 106 Terman says:
"Thus, if the line is short-circuited at the load, then at frequencies
in the vicinity of a frequency for which the length is an odd number of
quarter wavelengths long, the impedance will be high and will vary with
frequency in the vicinity of resonance (i.e., frequency corresponding to
quarter wavelength) in exactly the same manner as does the impedance of
an ordinary parallel resonant circuit. It is therefore possible to
describe resonance on a transmission line in terms of impedance at
resonance and the equivalent Q of the resonance curve.

On page 107, Terman gives a 200 MHz example. 2-inch air-dielectric coax
is used for 1/4-wave short-circiuited stubs about 15 inches long. The
resonant impedance is more than 250,000 ohms with a Q of 3000.

How much current flows into an impedance of more than 1/4-million ohms?

Best regards, Richard Harrison, KB5WZI


Cecil Moore June 17th 04 02:03 AM

Richard Harrison wrote:
How much current flows into an impedance of more than 1/4-million ohms?


As you know, transmission lines transform impedances. That stub likely
has an SWR around 5000:1. Assuming a driving voltage of 250V, the
current at the 1/4-million ohm point is about 0.001 amps. However,
1/4WL away, at the short in the 1/4WL stub, the current will be
~5 amps with a voltage of ~0.05V. That's an impedance of ~0.01 ohm. The
shorted stub has transformed the impedance from 1/4-million ohms at
the mouth to ~0.01 ohm at the short. That's what transmission lines do.

The question is not, "How much current flows into an impedance of more
than 1/4-million ohms?" The question is: How much current flows 1/4WL
away from that point at the shorted end of the stub? The answer is the
sum of the forward current and reflected current. The voltage at the
shorted end of a 1/4WL stub is the difference between the forward voltage
and the reflected voltage.

The voltage at the mouth of the stub is the sum of the forward voltage
and reflected voltage. The current at the mouth of the stub is the
difference between the forward current and reflected current. In the
example above, that difference is ~0.001 amp. The forward current flowing
inside the stub is ~2.505 amps and the reflected current flowing inside
the stub is ~2.495 amps.

If you don't believe the above, simply measure the RF current at the
shorted end of the stub. Someone modeled it the other day and even
the modeling program indicated that the current was sky high at
the shorted end of a 1/4WL stub.
--
73, Cecil http://www.qsl.net/w5dxp



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Richard Harrison June 17th 04 03:37 AM

Cecil, W5DXP wrote:
"Someone modeled it the other day and even the modeling program
indicated that the current was sky high at the shorted end of a 1/4 WL
stub."

Agreed that the resistance of the short is small and allows a large
current even when the volts are low. The small load resistance, ZL is
transformed into another resistance, ZS that is inversely proportional
to ZL. Terman expresses this in equation (4-31) as:

ZS = Zo squared / ZL

So, the smaller ZL, the larger ZS. As ZL goes to zero, ZS goes to
infinity.

A high impedance means: accepts little current for a given voltage. The
open end of a good 1/4-wave short-circuited stub is defined as a high
impedance. So much so that it is also called a "metallic insulator".

Best regards, Richard Harrison, KB5WZI


Cecil Moore June 17th 04 05:17 AM

Richard Harrison wrote:
A high impedance means: accepts little current for a given voltage. The
open end of a good 1/4-wave short-circuited stub is defined as a high
impedance. So much so that it is also called a "metallic insulator".


If it was indeed a high physical impedance, like a 250K resistor, it could
be removed and no much would happen at its resonant frequency. Unfortunately,
it is not a physical impedance and is merely a V/I ratio, a virtual impedance.
There is nothing at the mouth of the stub capable of causing reflections.
All the reflections occur at the shorted end of the stub.

The forward and reflected voltages add in phase and the forward and
reflected currents add 180 degrees out of phase at the mouth of the stub.
The ratio of forward voltage to forward current is the Z0 of the stub as
is the ratio of reflected voltage to reflected current.
--
73, Cecil http://www.qsl.net/w5dxp



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