Why Doesn't a Transmission Line Radiate All Its Power Away?

In summary: With no antenna connected, measure the voltage across the resistor. With the antenna connected, measure the voltage across the resistor again. You should see a decrease in voltage because the radiation is being cancelled out.
  • #1
GhostLoveScore
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This question is about transmission line that I use between my Ham radio and the antenna.

We a transmission line that is made of two parallel conductors close together. The current in one conductor is exactly the same as the current in the other conductor, but flowing in opposite direction. Transmission line's impedance is 50 ohm and it is terminated into a 50 ohm load. In every text it says that their fields will cancel each other and there will be no radiation looking at some distance "d" that is much larger that two conductors separation.

That sounds logical but we still have two wave sources from those two wires. Even if their fields cancel each other at the distance they must still lose power due to the radiation.

So why doesn't the transmission line radiate all the power away?

There are no standing waves on the transmission line. Do we have to have standing waves in order to radiate something away? In that case, if we left transmission line not terminated, would it radiate since standing waves would occur on it?
 
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  • #2
GhostLoveScore said:
This question is about transmission line that I use between my Ham radio and the antenna.

We a transmission line that is made of two parallel conductors close together. The current in one conductor is exactly the same as the current in the other conductor, but flowing in opposite direction. Transmission line's impedance is 50 ohm and it is terminated into a 50 ohm load. In every text it says that their fields will cancel each other and there will be no radiation looking at some distance "d" that is much larger that two conductors separation.

That sounds logical but we still have two wave sources from those two wires. Even if their fields cancel each other at the distance they must still lose power due to the radiation.

So why doesn't the transmission line radiate all the power away?

There are no standing waves on the transmission line. Do we have to have standing waves in order to radiate something away? In that case, if we left transmission line not terminated, would it radiate since standing waves would occur on it?
There is radiation from each wire, but it almost cancels at some distance away because the wires are close together in terms of the wavelength. It can also be thought of as mutual impedance between the lines which reduces radiation. The line can be considered as two antennas mounted close to each other and driven in anti phase.
By the way, I would be surprised if you have a two wire line with a characteristic impedance of 50 ohms - it is more likely to be a few hundred.
If standing waves exist on the line, this means that the current will be exaggerated at some parts of the line and will increase the radiation, but as we have seen, it is still negligible. It is usually satisfactory to use an open wire line at very high VSWR, even 20 or 30 is still satisfactory, and allows the matching adjustment to be made at the transmitter end of the line, which is very convenient.
 
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  • #3
So how much does each wire radiate? Let's say that I have half wave dipole for 3.5MHz, that's 40m total antenna length. And let's say that I have 40m of open wire feedline. Let's say that open wire has impedance of 450 ohms and dipole has impedance of 75 ohms. How much would each wire in open wire feedline radiate?
 
  • #4
There should be a tiny dipole effect I think. The power loss would be insignificant, but you might try shielding if it starts to interfere with something.

But how could that be if you are driving an antenna a few meters away? The antenna would swamp any dipole effect. Still if one were building a radar isolated after the transmission line, it could be a problem.
 
  • #5
I don't really know how to explain this question better. I am feeding the dipole antenna with open wire feedline. Feedline does not radiate looking from the distance because currents in these two wires are the same amplitude but flowing in different directions. Does that mean that each wire is radiating EM radiation but when those two EM waves interfere they cancel each other? If that is true, how much each wire radiates?
 
  • #6
GhostLoveScore said:
So how much does each wire radiate? Let's say that I have half wave dipole for 3.5MHz, that's 40m total antenna length. And let's say that I have 40m of open wire feedline. Let's say that open wire has impedance of 450 ohms and dipole has impedance of 75 ohms. How much would each wire in open wire feedline radiate?
I would think you would have more problem with near field coupling than with radiative losses.

Still, to measure the radiation (far field effect), attach a dummy load and measure the radiation pattern far from the line (at least 10 wavelengths, more is better).

We can't even begin to estimate such a small effect without knowing a lot more information including the ground plane, support structure, and other possible interferences.

Radiation is an effect of special relativity. It happens when charges accelerate changing their relatavistic reference frame. Antennas guide such accelerating charges while not providing easy ways for the emitted photons to reabsorb. Your transmission line fails that last requirement. Photons emitted by one wire are nearly exactly reabsorbed by the other.

The photons are very roughly equal to the wavelength in size, so much bigger than the distance between the wires. Most of them never had a chance to break free.

Near field effects are classical and follow Maxwell (as opposed to relatvistic Maxwell, BTW). Your emitted fields might cause currents in the ground for example which would then pick up I2R losses.
 
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  • #7
GhostLoveScore said:
I don't really know how to explain this question better. I am feeding the dipole antenna with open wire feedline. Feedline does not radiate looking from the distance because currents in these two wires are the same amplitude but flowing in different directions. Does that mean that each wire is radiating EM radiation but when those two EM waves interfere they cancel each other? If that is true, how much each wire radiates?
Radiation implies power which means moving energy. Technically neither wire has any energy (except resistive losses). The energy is carried in the electric and magnetic fields around the wires. The wires just act to guide these waves. As such, you question has little meaning.

We can divide the fields and their energy into components based on the changing (accelerating) currents, but that is an somewhat artificial division. Under this division, we can say one wire is handing energy off to the other. How much depends on how much energy you are pumping through the circuit. At some point in time, all of the current will be in each wire. At other times none. (It's AC after all.) However none of the energy is ever in either wire (except I2R losses).
 
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  • #8
So that means that dipole radiates because the two wires are 180 degrees apart and they can't absorb each others fields?
 
  • #9
GhostLoveScore said:
So that means that dipole radiates because the two wires are 180 degrees apart and they can't absorb each others fields?
No. Because they are out of phase, they almost "absorb" (more correctly "cancel") each others' fields.

The dipole effect is caused by the distance between the two wire. If the two wires were in exactly the same place, they would exactly cancel. Since they are separated they only almost cancel.

Suppose the wires are mounted flat, one next to the other (which is typical). Looking from above and at a distance, the fields exactly cancel. But from the side, one is slightly closer than the other. This makes it slightly stronger. So they don't exactly cancel in this direction.

There is a tiny opportunity for a photon to escape in this direction. But it will be many dB lower than in an antenna and directional to boot. Since it is near the antenna the effect will be unnoticeable for most purposes.
 
  • #10
What fields are we talking about, are we only talking about magnetic fields of two wires that's interacting or are we talking about EM waves from two wires with their magnetic and electric fields interacting?

EDIT: I think I understand. We are looking at total magnetic field from two wires. It doesn't matter that there are two wires that have two magnetic fields. What matters is total magnetic field which is near zero. Am I getting any closer?
 
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  • #11
GhostLoveScore said:
So that means that dipole radiates because the two wires are 180 degrees apart and they can't absorb each others fields?
In this case, the two wires are fed at opposite ends but 180 degrees out of phase, so the overall effect is additive i.e. in-phase radiation.
 
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  • #12
GhostLoveScore said:
What fields are we talking about, are we only talking about magnetic fields of two wires that's interacting or are we talking about EM waves from two wires with their magnetic and electric fields interacting?

EDIT: I think I understand. We are looking at total magnetic field from two wires. It doesn't matter that there are two wires that have two magnetic fields. What matters is total magnetic field which is near zero. Am I getting any closer?
Both the electric field and the magnetic field (which are typically 90º apart) add in a linear fashion. So the + electric field cancels the - electric field, and the north magnetic field cancels the south magnetic field.
 
  • #13
Jeff Rosenbury said:
Both the electric field and the magnetic field (which are typically 90º apart) add in a linear fashion. So the + electric field cancels the - electric field, and the north magnetic field cancels the south magnetic field.

You are not talking about destructive interference?
6acd38d48065ef988dddb89df4f1dd9c.png

That way we would have areas with no radiation and areas with radiation. That's obviously not how transmission lines work.

EDIT:
I mean, why would one wire "care" where the other wire is? If we pulled them apart so they look like a dipole it would radiate. If they are parallel they don't radiate. It's not interference because there is no interference pattern, and besides, if it was interference, all of the power would get radiated before it even reached the antenna.

I understand how magnetic fields can cancel each other, and how electric fields can cancel each other, but I can't understand how they can cancel each other in feedline when nothing is radiated away from feedline.
 
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  • #14
GhostLoveScore said:
You are not talking about destructive interference?

No. The points (wires?) above are λ apart. In your transmission line, they are close (typically 1/10 λ or less).
 
  • #15
GhostLoveScore said:
So how much does each wire radiate?
The amount that each one radiates is affected greatly by the current flowing in the other. You cannot consider them separately if you want to calculate the 'total power'.
One way of looking at it is that the two wires constitute a very thin loop antenna. Such an antenna is very badly matched free space so it will not radiate much power.
But a simple two wire feeder does produce finite radiation. The effect of this radiation can cause crosstalk between nearby open wire feeders (and audio lines) which can be partially canceled by reversing the connections every so often - and by twisting the pairs.
 
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  • #16
GhostLoveScore said:
You are not talking about destructive interference?
a%2Fscience%2Fgrade-11%2F06-2d-and-3d-wavefronts%2Fpspictures%2F6acd38d48065ef988dddb89df4f1dd9c.png

That way we would have areas with no radiation and areas with radiation. That's obviously not how transmission lines work.
That diagram is not appropriate here. A and B are a small fraction of a wavelength so the interference pattern will have a very shallow max and min. The absolute level will also be small because of the mismatch.
 
  • #17
Is there some book that you would recommend me to read about this?

Impedance of the free space is 377 ohms. we have open wire feedline with 350 ohms characteristic impedance. How can it be matched badly to free space?
The only thing that I can find that is different in the antenna is the shape of the electric field lines.

Untitled.png
Does it have to do with that?

OK, basically what I read was that in order for something to radiate, it must have radiation resistance. Radiation resistance depends on geometry of the antenna. So, two wire feedline doesn't have radiation resistance? Or should I say, very small radiation resistance?
 
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  • #18
I think the diagram which is, I think, by J D Kraus, is very misleading. It is not enough to just create a 377 ohm transmission line to obtain radiation. Sorry I cannot recommend a book which describes the process of radiation in a correct and simple manner.
 
  • #19
OK, can you at least confirm if this is correct?

We have two parallel wires and we are looking at some small length segment dL.
Is magnetic field from left wire segment inducing current in the right wire segment?
 
  • #20
GhostLoveScore said:
OK, can you at least confirm if this is correct?

We have two parallel wires and we are looking at some small length segment dL.
Is magnetic field from left wire segment inducing current in the right wire segment?
Yes. But once again it is a dipole-ish effect. (But for a different reason.)

Magnetic fields circle current carrying wires. This is so fundamental that the IEEE organization uses it as its symbol. Similarly circling magnetic fields induce a current.

So the first wire induces a field. But that field circles the first wire not the second. Instead the second wire feels a slight curl because the far side of the wire is farther away than the near side. So some current will be induced, but not much. Further the amount will depend on the thickness of the second wire.

On radiation resistance: Radiation resistance is how most antenna designers account for the relativistic effect of the photons jumping into space -- i.e. far field energy loss. Few texts wish to go into the relativity thing, so I doubt you will encounter it. It is highly dependent on morphology (as is the underlying relativistic effect). EEs like to think in fields rather than particles (both are valid and mathematically equivalent).
 
  • #21
tech99 said:
In this case, the two wires are fed at opposite ends but 180 degrees out of phase, so the overall effect is additive i.e. in-phase radiation.

See, that's what is confusing me. Your explanation suggests wave interference. But that would mean that even in transmission line, we would have to have two wave sources which destructively interfere with each other. That would mean we would need to spend energy to create those two waves.
 
  • #22
sophiecentaur said:
Such an antenna is very badly matched free space so it will not radiate much power

What is needed to make antenna matched to free space?

Can we at least look at open wire feedline as two parallel antennas and like my antenna picks up EM waves from another station could they "pick up" radiation from each other and "absorb" almost all of it?
 
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  • #23
"Impedance of the free space is 377 ohms. we have open wire feedline with 350 ohms characteristic impedance. How can it be matched badly to free space?"
The characteristic impedance of a transmission is the Resistance that, when terminating the line, produces no reflection. In between the transmission line and space is a radiating structure. The input impedance of a dipole can be anything (many combinations of resistive and reactive ) - depending upon its length and where it's fed. The fact that those two numbers are similar is not relevant. I think you are straying into a bit of numerology here. :smile:
 
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  • #24
GhostLoveScore said:
What is needed to make antenna matched to free space?
That's rather the wrong way round. It's the antenna (plus any matching matching network) that matches a transmission line to free space.
With a suitable matching network (transformer / inductor / capacitance top etc etc), it is possible to match into any structure (even a dead sheep - as an antenna installation colleague once remarked).
 
  • #25
OK, so you said that we can look at the transmission line as loop antenna, but in that shape it will be badly matched to free space. So I would like to re-formulate the question: What decides if the antenna will match transmission line to free space? Obviously the dipole antenna is a good match. Transmission line is not.

As I said before, is it because the EM wave from one wire in transmission line is inducing the current in other wire and being almost completely "absorbed" in the wire?
 
  • #26
GhostLoveScore said:
OK, so you said that we can look at the transmission line as loop antenna, but in that shape it will be badly matched to free space. So I would like to re-formulate the question: What decides if the antenna will match transmission line to free space? Obviously the dipole antenna is a good match. Transmission line is not.

As I said before, is it because the EM wave from one wire in transmission line is inducing the current in other wire and being almost completely "absorbed" in the wire?
¼λ.

There are many good antenna designs that don't use quarter wavelength conductor segments, but most of the easiest to understand do.

A half λ section gives lots of umph. A quarter λ driven conductor plus the image current in the ground plane often works out to be ½λ.

A full λ section tends to reabsorb it's own photons. ½ emits and the other ½ is 180º out of phase, so it absorbs.

There are lots of exceptions to this rule of thumb. Plus there are lots of caveats like remembering the physical wavelength varies with the dielectric or remembering gaps often count as much as conductors (slot antennas, etc.).

Yet ¼λ is a good rule of thumb.

Another rule of thumb: parts less than 1/10 λ can be ignored. Again, not always true, but it usually is. Thus your gap between wires of less than 1/10 λ makes a bad antenna. If the gap were bigger (like ½λ) that wouldn't be true. Then you would need to run the field equations to see what happens.
 
  • #27
GhostLoveScore said:
As I said before, is it because the EM wave from one wire in transmission line is inducing the current in other wire and being almost completely "absorbed" in the wire?
Not "absorbed" but almost cancelled. Any distant radiation in a direction normal to the plane of the thin loop will be zero because the E fields due to the two wires will be in opposite directions (perfect anti phase) and the H field will be 'outwards' and not transverse. In the plane of the loop there will be a small resultant E field because the phases of the two fields from each leg are not totally in anti phase because the distances are unequal. The fields in the vicinity of the loop are more complicated and the E and H fields are nearly in quadrature. As you get into the far field, the only result is E and H fields that are in phase (the radiated Em wave).

You are talking in terms of needing to supply energy for the radiation from each wire but the only energy that's involved is due to a failure of fields to cancel.
If you study antennae and transmission lines more deeply it becomes easier to see that the transmission line is a poor antenna and that a transmission line with a wide separation or a taper starts to be a better antenna and a worse transmission line. :smile: It's quite hard stuff, I think.
 
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  • #28
OK, I think that the my confusion was due to thinking that EM radiation is produced by each wire in transmission line. Instead EM radiation is produced by total magnetic and electric field from both wires, which is near zero. But that means that there is some minimum distance only after which E and H fields become free EM wave?
 
  • #29
GhostLoveScore said:
But that means that there is some minimum distance only after which E and H fields become free EM wave?

yes
this is the next step in the theory where you start looking at "near field" and "far field" processes

mutually couples inductors such as transformers use the near field inductive properties

Antennas make use of the far field radiative properties

time for you to do some reading :wink:

https://en.wikipedia.org/wiki/Near_and_far_field

http://electronicdesign.com/energy/what-s-difference-between-em-near-field-and-far-field

http://www.antenna-theory.com/basics/fieldRegions.php

there's 3 references out of 100's on google :smile:Dave
 
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  • #30
Ah, that's it. I thought EM wave is produced at conductor surface. Finally I can sleep :) And read about Near and far field tomorrow, thanks.
 
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  • #31
So after reading about near and far field I have few more questions.

From wikipedia:
Also, in the part of the near field closest to the antenna (called the "reactive near field", see below), absorption of electromagnetic power in the region by a second device has effects that feed back to the transmitter, increasing the load on the transmitter that feeds the antenna by decreasing the antenna impedance that the transmitter "sees". Thus, the transmitter can sense when power is being absorbed in the closest near-field zone (by a second antenna or some other object) and is forced to supply extra power to its antenna, and to draw extra power from its own power supply, whereas if no power is being absorbed there, the transmitter does not have to supply extra power.

In transmission line we have two wires. If I understood it correctly, in reactive near field, fields from each wire are absorbed by the other wire?
 
  • #32
GhostLoveScore said:
In transmission line we have two wires. If I understood it correctly, in reactive near field, fields from each wire are absorbed by the other wire?

No, any crap going on in the near field of the transmission line will affect it. This can be used to intentionally couple power or whatever, but mostly it just degrades the line. However because of the dipole effect the reactive nearfield is probably smaller in the transmission line than the average antenna. (Anything between the wires is messy though.)
 
  • #33
Jeff Rosenbury said:
No, any crap going on in the near field of the transmission line will affect it. This can be used to intentionally couple power or whatever, but mostly it just degrades the line. However because of the dipole effect the reactive nearfield is probably smaller in the transmission line than the average antenna. (Anything between the wires is messy though.)

But each wire in transmission line is in reactive near field of the other wire?
 
  • #34
GhostLoveScore said:
But each wire in transmission line is in reactive near field of the other wire?
Yes, but they are arranged to complement one another. They work together to guide the wave.

Random stuff in the near field messes with them working together. Metal acts as a conductor. Insulators act as dielectrics. (Many of which are close enough to εr = 1 to not matter, BTW.)

As I said, if it's intentional we can achieve lots of good things with add ons, like impedance matching or coupling power. It's when random things happen that things go down hill.

Have you considered taking a course in electromagnetics? You seem interested in the field.
 
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  • #35
Jeff Rosenbury said:
Yes, but they are arranged to complement one another. They work together to guide the wave.

Have you considered taking a course in electromagnetics? You seem interested in the field.

I have started studying physics in 2010, but I took a break in 2013. Hopefully I will continue this or next year. But yes, I would want to take courses in electromagnetics.

I know I can't understand it completely without looking into a math and equations, and I know that lot of weird stuff happens in near field of the antenna.
Can I at least look at it this way. There are two waves that are 180 degrees out of phase in the transmission line. Their fields cancel each other like this (b case)

image004.jpg


Not literally like in "b" case, just that part where their amplitudes cancel each other.
 
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