Can a crystal radio detect an infinitesimal load at a distant radio station?

In summary, the conversation discusses the possibility of detecting an infinitesimal increased load at a radio station when using a crystal radio set to tune in to a station 100 miles away. The consensus is that there would not be an increased load as the energy from the transmitter is still radiated away, but there may be a small signal radiated back to the transmitter from a resonant tuned circuit with an antenna on it. This is called a "passive reflector" and would only be detectable if the transmitter was turned off. There is also a discussion about the concept of a receiver drawing power from a transmitter, and the mutual impedance between transmit and receive antennas. The conversation ends with a mention of Nikola Tesla and his understanding of this topic
  • #36
Yes, but that wasn't the point of it. The point was that the radiated power is not zero when the matched condition exists.
 
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  • #37
The statement at issue was my claim that the re-radiated power is not only non-zero, it is equal to the absorbed power.
 
  • #38
If the antenna feedline looks like 50 ohms, then this maximum power will be delivered to the feedline.
If there were no losses, this power would also be delivered to the antenna and all of it would be radiated.

The above is the part I am interested in. When a transmitter drives a properly matched antenna system there is nothing the transmitter see differently than if the transmitter drives a resistor. So, we can assume that as VK6KRO has said ALL of the power the transmitter delivers to the antenna is radiated accept some loss which we will consider negligible. So why should the reverse not be true? Am I looking at this wrong? I've never really considered this before.
 
  • #39
I don't mind analyzing what goes on in a transmitter station, but I'm pretty sure it's going to be really really unhelpful in trying to understand how you absorb power with a receiving antenna. I was pretty serious when I said that it would be equally helpful to go into your living room and try and analyze a lamp cord as a transmission line, with reflections and standing waves. Technically it can be done, but to what end??
 
  • #40
conway said:
The statement at issue was my claim that the re-radiated power is not only non-zero, it is equal to the absorbed power.

I missed that in the exchange while I was typing my replies, but intuitively it seems very elegant. You mean the power absorbed into the matched load, I guess.
Pending a proper proof, it seems feasible.

So, we agree that a receive antenna can reradiate some or most of its received signal?

You might like to rephrase this though:
I don't actually know what the wasted power is in a 10-kW AM radio transmitter, but there's no technical reason why you'd want to match the amplifier impedance to the load.
This is not like loading a power station until its output voltage dropped to half. RF power amplifiers really do operate like this and impedance matching is very important with them.

Receive antennas are not normally matched for maximum power transfer. They are presented with a higher impedance than that, to achieve higher voltage into the receiver.

The above is the part I am interested in. When a transmitter drives a properly matched antenna system there is nothing the transmitter see differently than if the transmitter drives a resistor. So, we can assume that as VK6KRO has said ALL of the power the transmitter delivers to the antenna is radiated accept some loss which we will consider negligible. So why should the reverse not be true? Am I looking at this wrong? I've never really considered this before.

The comparable situation while transmitting would be that the antenna that is transmitting also receives the transmitted signal. I suppose it does, but I can't think how you would prove it.
 
  • #41
I think I have a good counterargument to an RX antenna (well matched) re-radiating anything. If it did, then antenna array steering would be much more complicated (if not impossible), which it isn't.

In antenna arrays, we phase shift the RX signals to steer the direction of the gain lobe. For a 2-element array, you can steer the direction of the gain lobes by phase-shifting the RX signals before combining them. And if you don't phase shift them, you get your lobes right where you expect them, front-to back, with gain determined by the RX signals only, not mitigated by some reflected energy passing between the two elements. We use this every Field Day, and antenna array equations are pretty well understood.

Whew. Glad that's settled!
 
  • #42
berkeman said:
I think I have a good counterargument to an RX antenna (well matched) re-radiating anything. If it did, then antenna array steering would be much more complicated (if not impossible), which it isn't.

This is logical, but remember you're talking about practical receivers where the antenna current is only a tiny fraction of the theoretical matched current.
 
  • #43
vk6kro said:
You might like to rephrase this though:
I don't actually know what the wasted power is in a 10-kW AM radio transmitter, but there's no technical reason why you'd want to match the amplifier impedance to the load.
This is not like loading a power station until its output voltage dropped to half. RF power amplifiers really do operate like this and impedance matching is very important with them.

I'd like to concede this point...but I still have to wonder. I looked up the Wikipedia article on electronic amplifiers and it's a huge topic. It's true that RF amplifiers operate in a mode where a large portion of the power is dissipated in the output stage, but it's not totally clear to me that impedance matching is the reason for this. To some extent it appears to be just the practicalities of transistor amplifier design. For a radio transmitter station, I can't see any reason why the designer wouldn't want to put the maximum percentage of the available power into the transmitted wave. I stand to be corrected on this point if possible.
 
  • #44
conway said:
This is logical, but remember you're talking about practical receivers where the antenna current is only a tiny fraction of the theoretical matched current.

Nope. True at any RX E&M level. Field tested. That's why it's so helpful in this thread.
 
  • #45
For a radio transmitter station, I can't see any reason why the designer wouldn't want to put the maximum percentage of the available power into the transmitted wave.

That is exactly what designers are trying to do. Power transistors and RF power tubes as used in transmitters are expensive and it makes sense to get as much power out of them as possible.

However, the realities of power stage design mean that efficiencies of only 50% are possible in some modes (SSB linear amplifiers) and up to 70 % in other modes (Class C CW transmitters).

You might wonder why anyone would use an amplifier that only has 50 % efficiency but that is only while the user is talking. When they take a breath, the power used is negligible.
 
  • #46
GODISMYSHADOW said:
Someone should establish some rules for "thought experiments."
You're talking about astronomical distances. Here, you take sides
with the receiver and switch to the viewpoint of the transmitter.
Then you jump back to the receiver. Seems dangerous to me,
because information itself can't travel faster than light. I don't like
your thought experiment.
I took issue with the notion of a RX antenna "drawing power" from a TX antenna when they are well separated. Naturally, when they are close, their mutual impedance can affect the input impedance of the TX antenna (as in a Yagi type array, with parasitics) but any model which implies the "drawing out" process at great distance should work over any distance - hence, I took it a bit further to where propagation time is a significant factor. As a thought experiment I don't think it was over the top to consider ("take sides with") both RX and TX; after all, they are both involved in the process. Where was the problem with that?.
 
  • #47
berkeman said:
I think I have a good counterargument to an RX antenna (well matched) re-radiating anything. If it did, then antenna array steering would be much more complicated (if not impossible), which it isn't.

In antenna arrays, we phase shift the RX signals to steer the direction of the gain lobe. For a 2-element array, you can steer the direction of the gain lobes by phase-shifting the RX signals before combining them. And if you don't phase shift them, you get your lobes right where you expect them, front-to back, with gain determined by the RX signals only, not mitigated by some reflected energy passing between the two elements. We use this every Field Day, and antenna array equations are pretty well understood.

Whew. Glad that's settled!

Actually, that only applies to active receiving arrays. For a number of elements, situated close to each other, if you want to direct the main beam by passive phasing of the outputs, the element currents will affect each other (more of the mutual impedance matrix values become significant). The local (resonant / reactive) fields around the elements (E and H in quadrature at this point) can be quite significant and they talk to each other*. Many active arrays deliberately use 'voltage probe' elements rather than matched elements so that you can control them without needing to account for their effect on each other. Steering multi-element TX arrays is a real problem because you need to shift as much actual power from each element as possible. Try designing a simple steerable two element mf mast array with 1/2 wave spacing. For some beam angles the matching / driving is very hard.

*Things seem to change from I and V in a dipole and associated fields, which are in quadrature and E and H fields in the distant radiated wave, which are in phase.
 
  • #48
Matching:
To get the maximum signal power radiated, you have to match your TX to the antenna. That means you just have to put up with the fact that the output TX stage 'wastes' a lot (half) of the power.
For supplying electricity, you want just the opposite. You need power to be delivered with as little power as possible wasted in the generator / distribution. You would ideally have a 'voltage source'. The last thing you want is a matched system in the National Grid.
 
  • #49
I hope Berkeman agrees that Sophie's explanation takes care of his paradox with the receiving arrays. It's always impressive to me when people can show how the practical world lines up with the theory.

I'm not sure we've totally reached consensus on the question of impedance matching at the transmitter station. It's not clear to me from various postings whether the wasted power is on account of intentional impedance matching or just a practical fact of high frequency amplifier design.
 
  • #50
sophiecentaur said:
Actually, that only applies to active receiving arrays. For a number of elements, situated close to each other, if you want to direct the main beam by passive phasing of the outputs, the element currents will affect each other (more of the mutual impedance matrix values become significant). The local (resonant / reactive) fields around the elements (E and H in quadrature at this point) can be quite significant and they talk to each other*. Many active arrays deliberately use 'voltage probe' elements rather than matched elements so that you can control them without needing to account for their effect on each other. Steering multi-element TX arrays is a real problem because you need to shift as much actual power from each element as possible. Try designing a simple steerable two element mf mast array with 1/2 wave spacing. For some beam angles the matching / driving is very hard.

*Things seem to change from I and V in a dipole and associated fields, which are in quadrature and E and H fields in the distant radiated wave, which are in phase.

Not true. Why are the reflector and director elements in a Yagi not terminated? If they were, your Yagi wouldn't work so well...
 
  • #51
To maximise the power delivered from the feeder into the antenna you need to match at the drive point - that's straightforward enough and you try to minimise your VSWR / reflection coefficient at the join.
To get power actually into the feeder from the transmitter there has to be some degree of matching. A low impedance output stage will not drive much power into a high impedance load without using massive voltages - and vice versa. But, as you imply, conway, there are practical limits to how well you can match a (probably non-linear) amplifier stage and there will be inherent losses in the device in any case. I don't think that there are any particular design problems for 'bog standard' frequency operation, these days. They seem to build big HF transmitters a bit like audio amps these days - class B push pull blah blah.
To avoid echoes, over voltage and or odd frequency response, it is necessary to match at least one end of a feeder.
 
  • #52
berkeman said:
Not true. Why are the reflector and director elements in a Yagi not terminated? If they were, your Yagi wouldn't work so well...
A Yagi antenna is not steerable - it is designed to have lots of current in its parasitic elements in order to to drive it in one particular direction. It has only one driven element and it is not what I was describing. To steer with two or more driven elements is the problem. Then the mutual impedance between two elements is a nuisance. You can end up chasing your tail if you want to fire in certain directions.
 
  • #53
sophiecentaur said:
A Yagi antenna is not steerable - it is designed to have lots of current in its parasitic elements in order to to drive it in one particular direction. It has only one driven element and it is not what I was describing. To steer with two or more driven elements is the problem. Then the mutual impedance between two elements is a nuisance. You can end up chasing your tail if you want to fire in certain directions.

I was referring to the Yagi in RX mode, not TX. I thought that's what was in question -- whether there is a transmitted field from a well-matched (terminated) antenna when it is receiving a signal.
 
  • #54
I think we must be at cross purposes here. A Yagi has only one feed point (or 'driven point'), whether in transmit or receive mode and, as the two directivity patterns are indistinguishable, the relative currents in the elements must be more or less the same in each mode. The parasitics are, of course, 'short circuited' and not terminated. The Yagi only works with the elements around resonance. In the receive mode, the explanation for its operation must be that the parasitics resonate in similar relative phases to the driven element. Whether transmitting or receiving, this must take a few cycles to build up when the wave is first received or when the TX is turned on. After that, the currents in the elements are mutually set by the self impedances of the elements themselves and their mutual impedances with the other elements.
What has that got to do with the problems associated with multiple fed element antennae, though? The thread may have migrated here and there, as they do, but my comments were in response to comments about steering multi element arrays and the problems of currents flowing in elements affecting the current / input impedances of other driven elements. (The Yagi is not the only directive antenna and it certainly is not steerable - apart from by waving it around)
 
  • #55
I was using the example of an RX Yagi to try to make the point that you only get reflections off of unterminated antennas (shorted in this case), not off of terminated antennas (which I think is what conway has been saying. It seemed a convenient example. A Yagi with terminated directors and reflector would not be any more directional than a regular dipole.

And I brought up the example of steerable RX antenna arrays for the same reason. In RX mode, I'm not aware of any interaction between the antennas (no reflected signal bouncing between the elements and needing to be taken into account in the pattern calculation).

Sorry if I haven't been clear about why I was using these examples.
 
  • #56
I getcha now. But the fact is that, although there are higher currents in parasitics, there are still currents in driven elements (TX or RX) and these have mutual effects. If you ignore them, your antenna just won't do what you want it to do. If it is a TX array, you can end up with transmitter matching problems as well as a wrong pattern and, if it is an RX array, the pattern goes to pot.
 
  • #57
I hate it when people start off by saying "even if you're right..." because its a big cop-out: you're not even taking a stand on whether he's right or wrong. But in Berkeman's case I don't see that I have any choice: "even if he's right" about how you steer a receiver array, it's a really indirect connection to the original question of a crystal radio, which involves a single electrically short dipole. So whether he's right or wrong I don't think he can claim to have dealt with the question of how much re-radiation there is in a tuned matched short dipole.
 
  • #58
However short the dipole is, there will be currents flowing in it - in phase and out of phase with the PD. These currents will radiate. It will only be the real part of the current and PD that will be absorbed by the receiver. Matching the short dipole will involve other reactive components to resonate with the capacity that the short dipole represents and to transform to the receiver input impedance. In practice, you can only go so far down that road and the radiator gets less efficient due to the finite resistance of the conductors for really short radiators.
Just think how hard it is to make a 'stealth' aircraft. If it were simply a matter of making an aircraft surface look like a set of matched dipoles then they would be built like that. They all re-radiate - which is why they have to be made with 'least worst' reflecting shapes.
Very short elements won't re-radiate much - and neither will they absorb much power. Arrays of very short elements can be treated as voltage probes because there is so little scattered power. (This accords with experience - even down to the sky being blue.)
The earlier quoted 2:1 ratio of currents for unmatched and matched termination (way back in the thread) seems to have been forgotten but it should be taken into consideration.
 
  • #59
Ya know, it doesn't really make a damn bit of difference. Any power that was reradiated had to be 'drawn in' by the antenna in the first place. For all I care every available amount of power that the transmitting antenna hundreds of miles away radiated could have been absorbed by a receiving antenna which would then have turned around and reradiated all but what we normally see at the feedpoint of an antenna.
 
  • #60
sophiecentaur said:
I took issue with the notion of a RX antenna "drawing power" from a TX antenna when they are well separated. Naturally, when they are close, their mutual impedance can affect the input impedance of the TX antenna (as in a Yagi type array, with parasitics) but any model which implies the "drawing out" process at great distance should work over any distance - hence, I took it a bit further to where propagation time is a significant factor. As a thought experiment I don't think it was over the top to consider ("take sides with") both RX and TX; after all, they are both involved in the process. Where was the problem with that?.


It makes me feel uneasy, because when you're at RX the latest news
you can possibly have about TX is limited to whatever transmissions
or other electromagnetic radiation you are receiving. This is the most
current knowledge you can possibly have. The same would be true
but in reverse if you were at TX. The region outside the "light-cone" is
called "elsewhere" and you cannot know about that in your "here-now"
with certainty but only as a probability. Even when you look up at the
stars, what you see is the most current knowledge available. Any more
current news would be outside the light-cone and only a probability as
far as you're concerned. Anyway, that's the reason I don't like thought
experiments where they jump around too much.

Perhaps RX and TX taken together can be considered a system and then
wait for the system to stabilize.
 
  • #61
I'm going to support Sophie on this issue. When the receiver is far away from the transmitter, it does not in any way "load down" the transmitter, and basically for the reasons Sophie said. Of course there is a very small reflected wave but that's not what we mean by loading, even in principle. The energy transfer from A to B does not depend on the detection of the reflected wave; the receiver and transmitter would work exactly the same if the reflected wave could somehow be caught and destroyed before it got back to the transmitter.
 
  • #62
conway said:
I'm going to support Sophie on this issue. When the receiver is far away from the transmitter, it does not in any way "load down" the transmitter, and basically for the reasons Sophie said. Of course there is a very small reflected wave but that's not what we mean by loading, even in principle. The energy transfer from A to B does not depend on the detection of the reflected wave; the receiver and transmitter would work exactly the same if the reflected wave could somehow be caught and destroyed before it got back to the transmitter.

And I disagree with your reflected wave concept for a well-terminated RX half-wave dipole antenna, at least for now. We can agree to disagree, until one of us comes up with the math or an experiment to settle that, okay?
 
  • #63
I have a feeling that there is some confusion about how an antenna works. It isn't just the metal bits out there in space that are responsible for the power going in or our. An infinitely / very thin wire has more or less the same energy gathering properties as a fat wire. (Width helps to make the bandwidth of the element wider, but that's all) So the antenna must be working due to the fields surrounding it, which can be regarded as being caused by currents flowing in the conducting bit. These fields can be regarded as coupling energy into the feedpoint of the antenna. So why should it be suggested that, just because the antenna is matched, these fields should suddenly have no effect on the passing wave? You can, in principle and in practice, feed a wire anywhere you like - not just its mid point - and have a perfect match.

I was trying to think of an analogous situation and I suggest that a light disc shaped float, floating on the sea would be suitable. If it can float up and down on the waves without taking any energy then, if it were light enough, you would get no significant scattered energy from it. However, if you attempt to take energy from it - using it to pull on a crank, for instance, the float will no longer move directly in step with the water and this will involve waves emanating from it. You could imagine an appropriate value of friction (resistance) applied to the crank that would take a maximum of energy from the system - the waves would still be disturbed; you wouldn't imagine that, suddenly the waves would go past without being affected. So taking energy has involved disturbing the waves. Coupling the float to an appropriate resonating mass / spring system (without loss - representing a resonant length of wire) could produce greater movement of the float and, hence, more scattered waves. But in both cases there will be disturbance. The only time there is none would be when the float is not altering the power flow at all.
 
  • #64
OK, I don't think the math is normally helpful in these kinds of discussion, but here goes:

Take an AM radio station putting out a signal of 377 mV/meter (that's a pretty strong signal, obviously I picked the numbers so that the power density would be ExH=377 microvolts per meter squared). Let the station be at 680 kHz, wavelength approx 440 meters. Let your antenna be an 11 meter dipole. (No ground. Assume there is no ground.)

Now let's go to Wikipedia (http://en.wikipedia.org/wiki/Dipole_antenna) and look up the radiation resistance for a short (L/Lambda=1/40) dipole. Paraphrasing slightly:

R = approx 200 (L/lambda)^2 which gives in this case 0.125 ohms. To match the radiation resistance we use an appropriate coil to cancel the reactance of the antenna and insert a load resistance equal to R. The antenna voltage is ExL = approx 4 volts and the current is therefore 4 volts / 0.25 ohms = 16 amps.

The power to the load is I^2*R(load) = 32 watts and the power re-radiated, substituding R(rad) for R(load), is obviously the same.
 
  • #65
The sums have sorted it out, as usual. Thanks conway.
 
  • #66
As usual? It's rare that anything ever really gets sorted out in these kinds of discussions. I wouldn't write this one off yet either...
 
  • #67
I have to say I was wondering if anyone thought my numbers were unrealistic.
 
  • #68
Near enough to make the point.

The point seems to be that matching your antenna feed is not the same as replacing an area in space with a 'hole' for energy to flow out of, which is indistinguishable from the rest of the sphere into which the power is radiating. It is more like hanging a load half way along a long, perfectly terminated transmission line. You can get a optimum level of power into the load but that will, inevitably, produce a reflection / mismatch on the line at that point.
 
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