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Constructive interference in radiowave propagation
Cecil, W5DXP wrote:
"Antenna gain over isotropic is an application of constructive interference." Yes. An often offered annalog is an inflated spherical balloon. It contains the same amount of air no matter how it is squeezed. Sqeeze it one place and it bulges elsewhere. An isotropic antenna, could one be constructed, would radiate equally well in all directions. As a radiation pattern becomes lopsided, the bulge is filled with the energy squeezed from elsewhere. Directive gain of an antenna is a power ratio. It`s the power that you would have to put into an isotropic wersus the power you have to put into the gain antenna to lay the same signal on a point in the preffered direction. Other things equal, if a gain antenna radiates twice the power in the preferred direction as an isotropic, it has a gain of 3 dBi. Best regards, Richard Harrison, KB5WZI |
Constructive interference in radiowave propagation
Cecil Moore wrote:
Jim Kelley wrote: Then your observation was unrelated to the topic of discussion, which was your claim that 2 Joules per second could be obtained from a 1 watt laser. You know that I never claimed that, Jim. As bright a guy as you are, why do you have to stoop to falsifying what I have said? So now you start with the accusations, and here's why (from yesterday): "If it were total constructive interference, two 1/2W beams would yield an intensity of 2 watts." It was pointed out to you that that notion violates conservation of energy, but rather than admit that you were incorrect, you attempt to revise history. Then there was this: Hint: (2 watts/in^2 + 0 watts/in^2)/2 in^2 = 1 watt :-) Actually, it's a beam of light that subtends a solid angle of less than one degree. Let's call it a degree just to be conservative. That would leave 719 other solid degrees where there is 0 watts, so according to Cecil's theory of spacial power averaging, the answer could also be 2 watts+0+0+0... / 719 = 2.78 milliwatts. But apparently those values don't give the answer you were going for. Others have made points along these lines quite eloquently. Excellent comments in this thread from Roy, Keith, Owen, Gene, Tom, et al. 73, Jim AC6XG |
Constructive interference in radiowave propagation
Keith Dysart wrote:
Now just above, you started with 100W + 100W and ended with 400W. And you wonder why readers think you advocate this position. 100W + 100W is not all we started with. Somewhere else is 100W + 100W of destructive interference that adds up to zero. This is very much like the equation in Born and Wolf. Itotal = 4I1 where I1 = I2 = 100 watts/unit-area Such is the nature of constructive interference. That you are ignorant of such is noted. Does this not cause you some discomfort? It clearly violates conservation of energy. Absolutely NOT! There is 200 watts of destructive interference somewhere else. Here is a real-world example: ---291.4 ohm line---+---1/2WL 50 ohm line---291.4 ohm load Pfor1=200W-- Pfor2=400W-- --Pref1=0W --Pref2=200W On the load side of point '+': P1 = Pfor1(1-rho^2) = 100W P2 = Pref2(rho^2) = 100W P1 + P2 + 2*SQRT(P1*P2) = Pfor2 = 400W (200W of constructive interference) On the source side of point '+': P3 = Pfor1(rho^2) = 100W P4 = Pref2(1-rho^2) = 100W P3 + P4 - 2*SQRT(P3*P4) = Pref1 = 0W (200W of destructive interference) -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
Keith Dysart wrote:
Any example where reflected energy is allowed to reach the source cannot be analyzed in any valid real-world way. A strange assertion. Consider two wire phone lines; transmitter and receiver at each end. Consider cable modems; ditto. Consider computer busses; ditto. We are discussing ham radio sources, Keith, which are none of the above. How many hams use cable modems for their RF transmissions? Please get real. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
Jim Kelley wrote:
w5dxp wrote: If it were total constructive interference, two 1/2W beams would yield an intensity of 2 watts. That should have been 2 watts per unit-area. Note that I did NOT say two 1/2W beams would yield a power of 2 watts. The correct dimensions of intensity would be 2 watts/unit-area, a power density, not a power. I have already apologized for that goof in dimensions. It was pointed out to you that that notion violates conservation of energy, but rather than admit that you were incorrect, you attempt to revise history. Then there was this: No, that notion *DOES NOT* violate the conservation of energy principle which cannot be violated. That notion relies upon one watt per unit area of total destructive interference occurring somewhere else. The one watt of destructive interference causes a flat black area. The energy from that flat black area is redistributed to the area of constructive interference and causes that area to be twice as bright as the average area. Born and Wolf's equation is valid. Itotal = 4I1 where I1 = I2 = 0.5W 2 watts/unit-area = 4(0.5) watts/unit-area Again, I ask you to please cease from trying to twist my words into a violation of the conservation of energy principle. If you think I have uttered such words, you are mistaken. Next time you are confused, instead of your arrogant ASSumptions, please just ask me what I meant. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
"K7ITM" wrote in
ps.com: Hi Owen, I had a quick look at your article. Though I didn't try to proof-read it for accuracy, I was reminded that the equations I posted those long years ago said that if you know the _instantaneous_ voltage and current at a point on a line, and know its impedance (as a frequency- independent quantity), the equations apply, and you can resolve that instantaneous pair of values into forward and reverse. That's something that's not immediately obvious when people think only about sine waves. Tom, Something else that follows from the derivation is that whilst the indicated Pf and Pr do not have stand along meaning, Pf-Pr does have meaning irrespective of the nominal R for which the instrument is calculated. For example, if we cascade a 100W source, 50 ohm directional wattmeter, a 75 ohm directional wattmeter and a 100+j0 load, the instrument readings should be: - 75 ohm: Pf=112.4, Pr=12.4, P=100 - 50 ohm: Pf=104.1, Pr=4.1, P=100 This of course assumes that the instruments do not significantly disturb the thing they are measuring, in this case the V/I conditions at the 100 ohm load. So, while you can nominate any reference Zo for a Pf or Pr value (and so vary those values), the power passing the instrument (Pf-Pr) is indicated correctly irrespective of the calibration R. (The article explains that the result of Pf-Pr is only meaningful if the calibration impedance is purely real.) Owen |
Constructive interference in radiowave propagation
On Apr 10, 4:13 am, "Keith Dysart" wrote:
Why don't you analyze my example: (Since the Grand PoohBah Power Master seems unwilling, here, for your consideration, I give you...) Generator with 291.4 Ohm ------------ 291.4 Ohm line ---- 50 Ohm load Source Impedance Pfor2=100w-- --Pref2=50w What is the power emitted by the generator into the line? -- Assuming lossless line, 50W of course; 50V@1A at the load. Where does Pref2=50W go? -- Into satisfying the boundary conditions at the generator to line interface. We have way to little info to determine if the generator dissipates more, or less, or the same, as if it were terminated in 291.4 ohms. Are there ghosts? -- Some people believe in them. I've never seen on--Oh not THAT kind of ghost. Well, not at the load, but certainly at the generator, if the generator is putting out a signal that's an interesting enough function of time. TDRs really do work. What is the magnitude? -- Of what? We have enough info to resolve Vf, If, Vr and Ir on the line, and if we knew the line length and the excitation, we could be a lot more definitive about things, but since steady-state excitation doesn't produce ghosts... but the reflection coefficient at the line-load interface is -1/sqrt(2), so that's the voltage ratio we'll see between the forward and reverse waves. What power would the generator emit if the line was terminated with 291.4 Ohms? -- "100 watts, of course." For those who don't immediately see that, it's not difficult to go through some math to show that the power delivered to a load is independent of the load impedance so long as magnitude((Zload-Rgen)/(Zload+Rgen)) is constant--that is, so long as the magnitude of the reflection coefficient is constant--as it is along a lossless line... and from that, find the Thevenin or Norton equivalent of the source in this example ... and from that, figure the power that source will deliver to a matched load. Please do not modify the example for analysis since this may change the results. There is much to be learned by trying examples that may challenge your expectations. :-) This reminds me of some thoughts I posted a long time ago about lines whose Zo is somewhat reactive. For example, if a linear sinusoidal source of impedance Zo is connected to a line also of impedance Zo, what load maximizes the power in the load? If you keep magnitude((Zload-Zo)/(Zload+Zo)) constant, is the power dissipated in the load independent of the phase angle of (Zload-Zo)/(Zload+Zo)? ...Keith Cheers, Tom |
Constructive interference in radiowave propagation
On Apr 10, 4:46 pm, Cecil Moore wrote:
Keith Dysart wrote: Any example where reflected energy is allowed to reach the source cannot be analyzed in any valid real-world way. A strange assertion. Consider two wire phone lines; transmitter and receiver at each end. Consider cable modems; ditto. Consider computer busses; ditto. We are discussing ham radio sources, Keith, which are none of the above. How many hams use cable modems for their RF transmissions? Please get real. Are you sure there are different rules for ham radio sources than for all the other ones? Something different about them? Something that makes them not amenable to the techniques used for others? If that is so, I am surprised at your claim that ham radio sources have something in common with light bulbs and lasers such that knowledge of those subjects can help analysis, while any knowledge of the behaviour of other electrical circuits is for naught. Seriously though, it does all work. The problems are solvable. You don't need to throw up your hands and say: "too tough." And then rationalize this response by calling them "too different" or saying "insufficient information". Much can be learned by solving the problems set using more controlled examples. Try it. Using the regular techniques will produce the same answer for all the problems you can currently solve, as well as allowing you to solve ones you currently declare as unsolvable. ....Keith |
Constructive interference in radiowave propagation
On Apr 10, 5:30 pm, "K7ITM" wrote:
On Apr 10, 4:13 am, "Keith Dysart" wrote: Why don't you analyze my example: (Since the Grand PoohBah Power Master seems unwilling, here, for your consideration, I give you...) Generator with 291.4 Ohm ------------ 291.4 Ohm line ---- 50 Ohm load Source Impedance Pfor2=100w-- --Pref2=50w What is the power emitted by the generator into the line? -- Assuming lossless line, 50W of course; 50V@1A at the load. Where does Pref2=50W go? -- Into satisfying the boundary conditions at the generator to line interface. This is a different way of expressing it. But I like it. We have way to little info to determine if the generator dissipates more, or less, or the same, as if it were terminated in 291.4 ohms. Are there ghosts? -- Some people believe in them. I've never seen on--Oh not THAT kind of ghost. Well, not at the load, but certainly at the generator, if the generator is putting out a signal that's an interesting enough function of time. TDRs really do work. What is the magnitude? -- Of what? I was think of the ghost, for those who believe in them, mostly to force some computation. If there is one, it must be quantifiable. We have enough info to resolve Vf, If, Vr and Ir on the line, and if we knew the line length and the excitation, we could be a lot more definitive about things, but since steady-state excitation doesn't produce ghosts... but the reflection coefficient at the line-load interface is -1/sqrt(2), so that's the voltage ratio we'll see between the forward and reverse waves. What power would the generator emit if the line was terminated with 291.4 Ohms? -- "100 watts, of course." For those who don't immediately see that, it's not difficult to go through some math to show that the power delivered to a load is independent of the load impedance so long as magnitude((Zload-Rgen)/(Zload+Rgen)) is constant--that is, so long as the magnitude of the reflection coefficient is constant--as it is along a lossless line... and from that, find the Thevenin or Norton equivalent of the source in this example ... and from that, figure the power that source will deliver to a matched load. There is much to be learned by trying examples that may challenge your expectations. :-) This reminds me of some thoughts I posted a long time ago about lines whose Zo is somewhat reactive. For example, if a linear sinusoidal source of impedance Zo is connected to a line also of impedance Zo, what load maximizes the power in the load? If you keep magnitude((Zload-Zo)/(Zload+Zo)) constant, is the power dissipated in the load independent of the phase angle of (Zload-Zo)/(Zload+Zo)? Hmmmmmm. I'll have to think on this. Perhaps after I work out whether the source impedance of a properly tuned amateur transmitter is the complex conjugate of the load impedance. ....Keith |
Constructive interference in radiowave propagation
Keith Dysart wrote:
Are you sure there are different rules for ham radio sources than for all the other ones? Something different about them? Something that makes them not amenable to the techniques used for others? You are using the rules of superposition in your examples. I don't know if the rules of superposition apply to those other sources but I do know that a ham transmitter, like my IC-706, is not linear enough to abide by the rules of superposition. How is superposition supposed to handle foldback? Ham transmitters cannot willy-nilly be shorted and opened in order to ascertain their linear model characteristics. A signal generator equipped with a circulator load solves all the experimental problems but doesn't act like a ham transmitter. Seriously though, it does all work. The problems are solvable. If that is true, why hasn't anyone ever solved them, published the results, and ended the arguments? The "solutions" produce different results depending upon whose brain is being used. Nobody has ever *solved* the problem and therefore the argument still continues to rage. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
On Apr 10, 4:41 pm, Cecil Moore wrote:
Keith Dysart wrote: Now just above, you started with 100W + 100W and ended with 400W. And you wonder why readers think you advocate this position. 100W + 100W is not all we started with. Somewhere else is 100W + 100W of destructive interference that adds up to zero. This is very much like the equation in Born and Wolf. Itotal = 4I1 where I1 = I2 = 100 watts/unit-area Such is the nature of constructive interference. That you are ignorant of such is noted. Does this not cause you some discomfort? It clearly violates conservation of energy. I see no connection between what you have posted above and what you posted below. Above: Itotal = 4I1 Below: nothing with a factor of 4 Above: 100 + 100 becomes 400 Below: 200 + 200 becomes 400 but then you compute a 100 and claim some relationship Absolutely NOT! There is 200 watts of destructive interference somewhere else. Here is a real-world example: ---291.4 ohm line---+---1/2WL 50 ohm line---291.4 ohm load Pfor1=200W-- Pfor2=400W-- --Pref1=0W --Pref2=200W On the load side of point '+': P1 = Pfor1(1-rho^2) = 100W P2 = Pref2(rho^2) = 100W P1 + P2 + 2*SQRT(P1*P2) = Pfor2 = 400W (200W of constructive interference) Now once again you have assumed that there are only positive roots. On the source side of point '+': P3 = Pfor1(rho^2) = 100W P4 = Pref2(1-rho^2) = 100W P3 + P4 - 2*SQRT(P3*P4) = Pref1 = 0W (200W of destructive interference) And positive roots here again, but this time it is subtracted. Isn't that the same as adding the negative root? So the two equations are identical, they just use the different roots. But how do you know which to use? Enquiring minds... ....Keith |
Constructive interference in radiowave propagation
Keith Dysart wrote:
Above: Itotal = 4I1 Below: nothing with a factor of 4 Look again. P1=100W, Pfor2=400W Above: 100 + 100 becomes 400 No, above: 100 + 100 + 2*SQRT(100*100) becomes 400 That's the nature of constructive interference. There is 200W of destructive interference on the source side of the Z0-match which is supplying the 200W of constructive interference on the load side. Now once again you have assumed that there are only positive roots. Since there is no such thing as negative power, the negative root is discarded as not representing reality. The sign of the interference comes from cos(0) for constructive interference and cos(180) for destructive interference. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
On Apr 10, 10:14 pm, Cecil Moore wrote:
Keith Dysart wrote: Now once again you have assumed that there are only positive roots. Since there is no such thing as negative power, the negative root is discarded as not representing reality. Isn't negative power just power that is going the other way? ....Keith |
Constructive interference in radiowave propagation
On Apr 10, 9:17 pm, Cecil Moore wrote:
Keith Dysart wrote: Are you sure there are different rules for ham radio sources than for all the other ones? Something different about them? Something that makes them not amenable to the techniques used for others? You are using the rules of superposition in your examples. I don't know if the rules of superposition apply to those other sources but I do know that a ham transmitter, like my IC-706, is not linear enough to abide by the rules of superposition. How is superposition supposed to handle foldback? One of the principles of superposition is that you can apply it to non-linear systems as long as they remain linear in the operating range that is of interest. Ham transmitters cannot willy-nilly be shorted and opened in order to ascertain their linear model characteristics. Read http://www.w2du.com/R2ch19.pdf and http://www.w2du.com/R3ch19a.pdf for descriptions on how to do so without needing to short or open the output. These articles argue that at least the amateur transmitters examined are linear over the operating range of interest. If that is true, why hasn't anyone ever solved them, published the results, and ended the arguments? The problems presented in the examples are solvable and have been solved in public on this group. The "solutions" produce different results depending upon whose brain is being used. Nobody has ever *solved* the problem and therefore the argument still continues to rage. The continuing argument is more a reflection on the people involved than on the problems. For the most part, the various approaches produce the same answer to the questions, except that some approaches provide no answer to some of the questions. Those who support those approaches then declare those questions unanswerable rather than exploring the approaches that do answer the questions. An interesting question is why do people reject the approaches that work without examination? I am sure that there must be some opportunities for psychological study there. ....Keith |
Constructive interference in radiowave propagation
Keith Dysart wrote:
Isn't negative power just power that is going the other way? I'm leery of the concept of propagating power (especially after seeing the morass it's led its adherents into), but most certainly negative power is the time rate of movement of energy that's going the other way. If we make a simple circuit of sine wave source and load where the load is anything but pure resistance, we can see that the energy goes one way for part of the cycle, the other way for the rest of half the cycle, then repeats the movement in alternate directions during the second half of the cycle. The powers (observed at a single point) during the movement in the two directions are positive and negative. Which direction of energy flow represents positive and which represents negative is entirely a matter of choice. The constant mixing of and confusion between power and energy is one of the tools used to keep the discussion's rational participants off balance, and it has been shown to work quite well. A real analysis of energy flow involves calculating the power at various points and times in the circuit or transmission line of interest. This gives a view of energy flow very different from the bouncing waves of average power; flurry of s-parameter gobbledigook; virtual shorts, opens, photons, and reflection coefficients; and vague parallels to optical phenomena that unceasingly issue forth. But the view that comes from calculation is correct, while the alternative is just so much smoke and noise. Roy Lewallen, W7EL |
Constructive interference in radiowave propagation
Keith Dysart wrote:
Isn't negative power just power that is going the other way? That is just a mathematical convention. If we say left to right is positive, then right to left becomes negative. If we say right to left is positive, then left to right becomes negative. Same for up/down or down/up or 45 degrees vs 225 degrees. It is a purely arbitrary mathematical convention. True negative power just doesn't exist. Negative energy would violate the conservation of energy principle. Is a Poynting vector pointing toward Alpha Centauri positive or negative? Since true negative power is impossible, the negative power result of a square root process is discarded as an artifact. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
Keith Dysart wrote:
One of the principles of superposition is that you can apply it to non-linear systems as long as they remain linear in the operating range that is of interest. One of the assumptions in your model is that the source impedance remains constant with varying degrees of incident reflected energy. That assumption is false for an IC-706. Variable constant source impedances are not allowed by the rules of superposition. The problems presented in the examples are solvable and have been solved in public on this group. :-) Then publish the results in QEX and settle it once and for all. :-) I predict that QEX will refuse to publish your ideas. The problems "solved in public on this group" are simple-minded and bear no resemblance to reality. They are akin to: Assume a lossless transmission line. Therefo There are no losses in transmission lines. In classical logic, your "solution" is known as petitio principii. An interesting question is why do people reject the approaches that work without examination? Translation: Why would anyone disagree with me and be wrong when they could agree with me and be right? :-) I am sure that there must be some opportunities for psychological study there. It's already been done. It's in the psychotic section under "delusions of grandeur". :-) -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
Roy Lewallen wrote:
A real analysis of energy flow involves calculating the power at various points and times in the circuit or transmission line of interest. Here's what I said years ago in my energy analysis article: "The term "power flow" has been avoided in favor of "energy flow". Power is a measure of that energy flow per unit time through a plane. Likewise, the EM fields in the waves do the interfering. Powers, treated as scalars, are incapable of interference." Seems you are still trying to influence people through false innuendo. ... flurry of s-parameter gobbledigook; There you have it, folks. Everyone give up on your S-Parameter analysis. It's only "gobbledigook" (sic). But the view that comes from calculation is correct, while the alternative is just so much smoke and noise. One wonders why that smoke and noise yields the same results as your short-cut methods plus the tracking of energy through the system. Could it be that the wave reflection model is a super-set of your simplified model? -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
Roy Lewallen wrote in news:131pgo519itfm24
@corp.supernews.com: .... I'm leery of the concept of propagating power (especially after seeing the morass it's led its adherents into), but most certainly negative power is the time rate of movement of energy that's going the other way. If we make a simple circuit of sine wave source and load where the load is anything but pure resistance, we can see that the energy goes one way for part of the cycle, the other way for the rest of half the cycle, then repeats the movement in alternate directions during the second half of the cycle. The powers (observed at a single point) during the movement in the two directions are positive and negative. Which direction of energy flow represents positive and which represents negative is entirely a matter of choice. Roy, one of the questions I continue to ask myself is why certain explanations of transmission line / load behaviour seem inconsistent with basic AC circuit theory as it applies at 50Hz or 60Hz, why the explanations hinge on a restriction that forward power and reflected power are purely real when in the general sense, a load may be reactive and therefore there is real and reactive power at the line-load interface, and similarly, depending on the transformed impedance, the source-line interface. One can only guess at the motivation for all the obfuscation that we see here. The invention of new terms, multiple meanings for terms, inconsistent properties for entities, switching in and out of optics, photon explanations, changing dimensions of quantities for convenience, construction of special cases to demonstrate assertions and that don't even qualify as inductive inferences, etc, are all part of a vast array of obfuscation. Thankfully, textbooks are not as confusing. Owen |
Constructive interference in radiowave propagation
Owen Duffy wrote:
Roy, one of the questions I continue to ask myself is why certain explanations of transmission line / load behaviour seem inconsistent with basic AC circuit theory as it applies at 50Hz or 60Hz, ... That's an easy one, Owen. The wavelength is so long at 60 Hz (5,000,000 meters) that the lumped circuit model usually works just fine. As you probably know, the lumped circuit model is a sub-set of the distributed network model. If the lumped circuit model worked for RF, the distributed network model (wave reflection model) would have been abandoned long ago. 100m of transmission line is 0.00002 wavelengths at 60 Hz. Distributed network effects are negligible. 100m of transmission line is 10 wavelengths at 30 MHz. Distributed network effects are at a 100% level. Current in the loop is flowing in opposite directions at ten points around the loop at the same time. Somewhere in between 60 Hz and 30 MHz, that old patched-up lumped circuit model must necessarily be discarded. One can only guess at the motivation for all the obfuscation that we see here. Sorry, but the actual obfuscation seems to me to originate with trying to use an inadequate, patched-up, lumped circuit model on distributed network problems. When the lumped circuit model yields correct results, the distributed network model yields the same results. When the lumped circuit model yields incorrect results, the distributed network model yields correct results. Again, the challenge is for you guys to generate standing- waves in the complete absence of reverse traveling waves. Until you provide a valid example of that, the reverse traveling waves continue to exist (in spite of all your hand-waving). They obey the rules of the wave reflection model and the principles of superposition and conservation of energy. The principle of superposition gives us permission to treat forward traveling waves and reverse traveling waves separately and then superpose the results. We get the correct answer every time. If you fail at generating standing waves without reverse traveling waves, then for what you guys say to be true, you must be able to generate traveling waves that contain zero energy. It appears that some people have been using mashed potato short-cuts for so long, they have lost track of the basic principles underlying the component wave behavior. Anyone who believes an S-Parameter analysis is "gobbledigook" (sic) falls into that category. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
On Apr 11, 7:41 am, Cecil Moore wrote:
Keith Dysart wrote: One of the principles of superposition is that you can apply it to non-linear systems as long as they remain linear in the operating range that is of interest. One of the assumptions in your model is that the source impedance remains constant with varying degrees of incident reflected energy. That assumption is false for an IC-706. Which is, of course, why all my examples explicitly state the construction of the generator to be one that is guaranteed linear. But if the behaviour for this kind of simple case can not be understood, there is no hope for understanding a real transmitter. The argument "since I can not understand a real transmitter, there is no value in understanding a linear generator" seems weak. The problems presented in the examples are solvable and have been solved in public on this group. :-) Then publish the results in QEX and settle it once and for all. :-) I predict that QEX will refuse to publish your ideas. I would hope so. The ideas are quite basic, not mine, and can be found in any standard text book on transmission lines and circuit analysis. No need to publish in QEX. Or perhaps I misunderstand QEX's audience and it is appropriate for them. But then I suspect that more capable writers than myself would be the appropriate authors. Have you considered putting optics aside for a moment (after all, we are trying to understand circuits, especially in the transmitter), and cracking open any textbook that deals directly with the subjects at hand? ....Keith |
Constructive interference in radiowave propagation
Owen Duffy wrote:
One can only guess at the motivation for all the obfuscation that we see here. Here's a list of questions for you and everyone else. 1. Is the distributed network model valid? If not, please explain where it is invalid. 2. Is the wave reflection model valid? If not, please explain where it is invalid. 3. Is the base of knowledge and laws of physics from the field of optics valid? If not, please explain where they are invalid. 4. Is an S-Parameter analysis valid? If not, please explain where it is invalid. 5. Does the principle of superposition give us permission to analyze the forward wave and reflected wave separately and then superpose the results? If not, please explain why not. 6. Does the conservation of energy principle work for forward and reflected waves? If not, why not? 7. Does the label of "obfuscation" really apply to items 1-6? 8. Do you and other gurus already know everything there is to know or does every person have holes in his/her limited knowledge base? -- 73, Cecil, w5dxp.com |
Constructive interference in radiowave propagation
"Cecil Moore" wrote in message t... Owen Duffy wrote: One can only guess at the motivation for all the obfuscation that we see here. Here's a list of questions for you and everyone else. 1. Is the distributed network model valid? If not, please explain where it is invalid. 2. Is the wave reflection model valid? If not, please explain where it is invalid. 3. Is the base of knowledge and laws of physics from the field of optics valid? If not, please explain where they are invalid. 4. Is an S-Parameter analysis valid? If not, please explain where it is invalid. 5. Does the principle of superposition give us permission to analyze the forward wave and reflected wave separately and then superpose the results? If not, please explain why not. 6. Does the conservation of energy principle work for forward and reflected waves? If not, why not? 7. Does the label of "obfuscation" really apply to items 1-6? 8. Do you and other gurus already know everything there is to know or does every person have holes in his/her limited knowledge base? -- 73, Cecil, w5dxp.com I have no beef with above, and would like to thank you and Walt for persisting in defending, explaining and trying to correct some "wrongos" out there. Seems that the unbelievers are in the same camp with those who could not digest the behavior of loading coils in standing wave antenna circuit. Seems it would be much nicer if the discussions were more in the line "oh, yea, why?" rather than "you fool, you know notin'" ...or something like that. I have experienced special case of interference between two antennas, fed from the same transmitter and separate amplifiers. The result was distorted signal on SSB, seems was a bit wider and modulation being raspy. It appears that part of the "other" RF was picked up by other antenna and amp, "processed" and retransmitted. I have observed this effect on one YU station, alerted him to it, asked to switch one PA-ANT off, and signal became "crystal" clean. Let the "it can't be" games begin :-) So it seems that if I want transmit the same signal in two or three different directions- antennas, they should not "see" each other, or they will interfere (until they go through atmo/ionosphere "massaging") and lose their correlating identity? Thanks Cecil and Walt! 73 Yuri, K3BU.us |
Constructive interference in radiowave propagation
Yuri Blanarovich wrote:
Seems that the unbelievers are in the same camp with those who could not digest the behavior of loading coils in standing wave antenna circuit. Seems it would be much nicer if the discussions were more in the line "oh, yea, why?" rather than "you fool, you know notin'" ...or something like that. If you remember, two of those gurus tried to use standing- wave current to measure the phase shift through a loading coil apparently not realizing that their simple-minded model wouldn't accomplish that task because the phase of standing- wave current is essentially unchanging all up and down the mobile antenna. Last I heard, they were rabidly defending those obviously flawed measurements because, of course, gurus know everything and never make mistakes. :-) -- 73, Cecil, w5dxp.com |
Constructive interference in radiowave propagation
On Apr 11, 4:14 am, Cecil Moore wrote:
True negative power just doesn't exist. Negative energy would violate the conservation of energy principle. Correct. Therefore 2*sqrt(P1*P2)cos(180) is impossible as well as ridiculous. Since true negative power is impossible, the negative power result of a square root process is discarded as an artifact. But what is TRUE negative power, and how does it differ from other types of negative power? :-) ac6xg |
Constructive interference in radiowave propagation
On Apr 11, 9:02 am, Cecil Moore wrote:
Again, the challenge is for you guys to generate standing- waves in the complete absence of reverse traveling waves. I do recall a textbook derivation of the voltages and currents on a trasmission line that used the distributed model and differential equations. It expressed the result in terms of x (distance along the line) and t (time). It was messy. It then followed this with a proof showing that thinking of the system as having a forward and reverse wave produced the same result. This was much simpler. But which one was real? In the end, it is the actual distributed voltage and current on the line that are real, not the means of describing them. Both methods accurately describe these, but I certainly prefer the latter since I can do the math for it. Still, just because I like to think of it that way, just because it gives me the right answers, does not mean that that is the way it is. Reality is the distributed voltage and current. Use the analysis technique of your choice, but only as long as it gives you the correct answers. ....Keith |
Constructive interference in radiowave propagation
Jim Kelley wrote:
Cecil Moore wrote: True negative power just doesn't exist. Negative energy would violate the conservation of energy principle. Correct. Therefore 2*sqrt(P1*P2)cos(180) is impossible as well as ridiculous. That's the interference term, Jim. Hecht, Born, and Wolf all agree that the interference term can be negative. Suggest you take a refresher course and alleviate the ignorance you are displaying for everyone to observe. Remember that P1 and P2 are Poynting vectors, i.e. power densities and the negative sign simply denotes the decrease in power density due to destructive interference. The negative destructive interference subtracts from the P1+P2 power and the result of that subtraction can *never* be negative. The interference term has NO separate existence aside from the existence of the power density components of P1 and P2. Please tell Hecht, Born, and Wolf that they are ridiculous. 2SQRT(I1*I2)cos(A) That's the third term in equation (15) page 259, 4th edition of "Principles of Optics". If cos(A) is 180 degrees, the interference term becomes negative and subtracts from the I1+I2 sum. Born and Wolf continue, "... and minima of intensity Imin = I1 + I2 - 2*SQRT(I1*I2)" Exactly the same equations appear in "Optics", by Hecht, 4th edition, page 388. "Imin = I1 + I2 - 2*SQRT(I1*I2)" Note that I is intensity or irradiance, the dimensions of which are watts/unit-area, exactly the same dimensions as the Poynting vectors, P1 and P2 above. In "Fields and Waves in Modern Radio", Ramo and Whinnery subtract Poynting vectors that are 180 degrees out of phase to obtain the net Poynting vector? Since true negative power is impossible, the negative power result of a square root process is discarded as an artifact. But what is TRUE negative power, and how does it differ from other types of negative power? :-) The sign on a power term denotes a decrease in power level but never to a negative level. Thus, reflected power subtracts from the forward power to obtain power delivered to the load. Destructive interference power subtracts from average power to allow for constructive interference power. In no case does the net power go negative. -- 73, Cecil, w5dxp.com |
Constructive interference in radiowave propagation
Keith Dysart wrote:
But which one was real? That's a metaphysical question. First please prove that you are real. :-) Use the analysis technique of your choice, but only as long as it gives you the correct answers. It has in every case so far. Other techniques, like using standing-wave current to try to measure the phase shift through a loading coil, have failed miserably. -- 73, Cecil, w5dxp.com |
Constructive interference in radiowave propagation
On Apr 11, 11:54 am, Cecil Moore wrote:
Keith Dysart wrote: But which one was real? That's a metaphysical question. So it is settled then. There is no NEED for a forward OR reverse travelling wave. Differential equations rule. First please prove that you are real. :-) It doesn't matter if I am real as long as you think I am. Use the analysis technique of your choice, but only as long as it gives you the correct answers. It has in every case so far. Well, except for the inability to explain where the "reflected power" goes in the transmitter. Of course this is not an issue for carefully selected examples where no "reflected power" reaches the transmitter. A more general analysis technique would not require such careful selection of examples. ....Keith |
Constructive interference in radiowave propagation
Keith Dysart wrote:
... Well, except for the inability to explain where the "reflected power" goes in the transmitter. Of course this is not an issue for carefully selected examples where no "reflected power" reaches the transmitter. A more general analysis technique would not require such careful selection of examples. ...Keith When I fire up the big russian 3.5KW linear into a high swr, I don't have to guess about where the reflected power is going at the xmitter, the nice red glow on the plates are an excellent indication when they begin dumping unknown amounts of power as infrared radiation ... when I grab the coax (150 ft. run) and feel its warmth, I even wonder about how much power it takes to elevate it's temp! JS |
Constructive interference in radiowave propagation
Cecil Moore wrote:
Jim Kelley wrote: Cecil Moore wrote: True negative power just doesn't exist. Negative energy would violate the conservation of energy principle. Correct. Therefore 2*sqrt(P1*P2)cos(180) is impossible as well as ridiculous. That's the interference term, Jim. Hecht, Born, and Wolf all agree that the interference term can be negative. Suggest you take a refresher course and alleviate the ignorance you are displaying for everyone to observe. Ah, but the ignorance being seen by all is all yours, sir. You continue to ignore a significant detail, Cecil. See if you can find it. Hint: people who write physics books know that power does not interfere. Please tell Hecht, Born, and Wolf that they are ridiculous. I agree with them, and they don't post here. But if they did, they'd be telling you the same thing as everyone else here. ac6xg |
Constructive interference in radiowave propagation
Keith Dysart wrote:
So it is settled then. There is no NEED for a forward OR reverse travelling wave. Differential equations rule. Yes, it is settled in your own mind. In my mind, there is certainly a need for forward and reverse traveling waves without which standing-waves would not be possible. If you want to deny the existence of the cause of standing-waves, there is nothing I can to stop you. Well, except for the inability to explain where the "reflected power" goes in the transmitter. Of course this is not an issue for carefully selected examples where no "reflected power" reaches the transmitter. A more general analysis technique would not require such careful selection of examples. The more general analysis technique tells us that the moon is 1000 miles away from the earth. I don't know how far away the moon is but I know it is not 1000 miles away. -- 73, Cecil, http://www.qsl.net/w5dxp |
Constructive interference in radiowave propagation
Jim Kelley wrote:
Hint: people who write physics books know that power does not interfere. Please tell that to someone who disagrees with that statement, Jim, which is not me. Here's what I said in my years old energy analysis article. "The term 'power flow' has been avoided in favor of 'energy flow'. Power is a measure of that energy flow per unit time through a plane. Likewise, the EM fields in the waves do the interfering. Powers, treated as scalars, are incapable of interference." You keep making statements like the above in hopes someone somewhere will believe that I disagree with it. Old trick - doesn't work. I say, *EM WAVES DO THE INTERFERING*. Do you want to argue about that? I say, *POWERS ARE INCAPABLE OF INTERFERENCE*. Do you want to argue about that? Please, if we are going to argue about something, make it something upon which we disagree. -- 73, Cecil, http://www.qsl.net/w5dxp |
Constructive interference in radiowave propagation
Cecil Moore wrote in
t: Owen Duffy wrote: Roy, one of the questions I continue to ask myself is why certain explanations of transmission line / load behaviour seem inconsistent with basic AC circuit theory as it applies at 50Hz or 60Hz, ... That's an easy one, Owen. The wavelength is so long at .... Cecil, you have conveniently clipped the context (as you do), the relevant context being the line-load interface and source-line interface. Statements in some explanations (by others) like "This clearly proves that reflected power and forward power in a transmission line are both real power, and that no fictitious power, or reactive volt-amperes, exists in either one." seem incompatible with the basic AC circuit theory explanation of a reactive load which must exchange reactive energy with the transmission line over a complete cycle (and the same effect at the source end). Perhaps it is explained by hopping in an out of the instantaneous and average context, just like switching between lossless lines and lossy lines context with declaration, while actually carrying the analytical simplicity of lossless lines and selectively layering selected aspects of the loss. BTW, I am not surprised at your dissertation apparently dismissing the distributed impedance model of a line, because after all it is the solution of that model that gives us the classic transmission line equations that you seem to not want to use. If the distributed network model you favour is the S paramater model, properly applied, it is in fact entirely consistent with the distributed impedance line model because the parameters are derived from the solution to the distributed impedance line model. Owen |
Constructive interference in radiowave propagation
John Smith I wrote in news:evj2m0$jb7$1
@nnrp.linuxfan.it: When I fire up the big russian 3.5KW linear into a high swr, I don't have to guess about where the reflected power is going at the xmitter, the nice red glow on the plates are an excellent indication when they begin dumping unknown amounts of power as infrared radiation ... when I grab the coax (150 ft. run) and feel its warmth, I even wonder about how much power it takes to elevate it's temp! John, With that insight and rigorous development, it must be time for you to publish a book. Owen |
Constructive interference in radiowave propagation
Owen Duffy wrote:
... John, With that insight and rigorous development, it must be time for you to publish a book. Owen Owen: How'd you guess? Title of book, "Spontaneous Thermal Emission of RF Finals and Feedline in Amateur Radio Systems With No Apparent Cause(s)!" Trouble is, the book stores keep putting it with the works on fiction :-( JS |
Constructive interference in radiowave propagation
Owen Duffy wrote in
: lines context with declaration, while actually carrying the analytical That should have read "without declaration". |
Constructive interference in radiowave propagation
Roy Lewallen, W7EL wrote:
"A real analysis of energy flow involves calculating the power at various points and times in the circuit or transmission line of interest." Yes. Bird Electronic Corporation has done a good job of this with its "Thruline" wattmeter for several decades. Its practice is to measure in a 50-ohm Zo resistive lossless impedance environment where forward and reflected waves are 180 regrees out-of-phase. This allows Bird to say: "Power delivered and dissipated in the load is given by: Watts into Load = Wforward - Wreflected" I would not argue with success. Best regards, Richard Harrison, KB5WZI |
Constructive interference in radiowave propagation
Richard Harrison wrote:
Roy Lewallen, W7EL wrote: "A real analysis of energy flow involves calculating the power at various points and times in the circuit or transmission line of interest." Yes. Bird Electronic Corporation has done a good job of this with its "Thruline" wattmeter for several decades. . . . No, the Bird wattmeter measures only the average power and only at one point. That's vastly different from what I described, which is instantaneous power as a function of time at many points along the line. A complete analysis of energy flow would include equations for the power as a function of time and position. You're sadly mistaken if you think you're getting this information from your Bird wattmeter. Roy Lewallen, W7EL |
Constructive interference in radiowave propagation
John Smith I wrote in news:evji53$kf9$1
@nnrp.linuxfan.it: Owen Duffy wrote: ... John, With that insight and rigorous development, it must be time for you to publish a book. Owen Owen: How'd you guess? Title of book, "Spontaneous Thermal Emission of RF Finals and Feedline in Amateur Radio Systems With No Apparent Cause(s)!" Trouble is, the book stores keep putting it with the works on fiction :-( John, it will never sell to the amateur market... you need a simple, catchy title. If it is destined for the fiction category, you could offer an sub title like "How reflections ruined my PA... from a ham who survived to tell the REAL story", with "Don't let it happen to you" emblazened in flouro red across the cover. Seriously, simple explanations are appealing, they provide content for discussion by experts on-air, whether they are correct or not. Simple explanations can be good, but incorrect ones are never good. Owen |
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