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Constructive interference in radiowave propagation
Roy Lewallen, W7EL wrote:
"No, the Bird wattmeter measures only the average power and only at one point." True. The Bird wattmeter measures average power, the same as any a-c wattmeter, and only at the point of measurement. If the line is lossy, the numbers are higher near the generator, and difference between forward numbers, for example, is an indication of loss between insertion points. Best regards, Richard Harrison, KB5WZI |
Constructive interference in radiowave propagation
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Constructive interference in radiowave propagation
Roy Lewallen wrote:
You're sadly mistaken if you think you're getting this information from your Bird wattmeter. Richard seems to be getting all the information from the Bird that he needs. However, your psychological compulsion to measure something besides average power is a perplexing need indeed. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
Cecil Moore wrote:
... Richard seems to be getting all the information from the Bird that he needs. ... Better to get 'yer information from the bird, then to be given the bird. Seems to be more than one bird "flying" around here! chuckle Regards, JS |
Constructive interference in radiowave propagation
On Apr 11, 1:06 pm, Cecil Moore wrote:
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. My mistake. But it is difficult to know your position when you don't indicate clearly that you disagree, so I thought that with your reply you were agreeing. Apologies. 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. This is a bit of a non sequitur. So what is it that you really disagree with in the analyses performed by myself and others? Just for clarity, an example problem that has been previously analysed is the following: A generator with a 450 Ohm source impedance drives a 450 Ohm ideal transmission line terminated in 75 Ohms. What is the magnitude of the re-reflected wave at the generator? I think you object to computing the amount of the reverse wave that is reflected at the generator by using the source impedance. More specifically you do not agree that the reflection coefficient at the generator can be derived using RC = (Zsource - Zline)/(Zsource + Zline). Also, you do not agree that superposition applies at the source. Given this, you then do not agree with the computations of the quantity of the reverse wave that is reflected at the source which then invalidates any further analysis. Have I managed to capture the essence of your disagreement with my and others analyses? Note that these analyses have been performed without the use of powers or interference so these side issues are not part of this question. ....Keith |
Constructive interference in radiowave propagation
Keith Dysart wrote:
My mistake. But it is difficult to know your position when you don't indicate clearly that you disagree, so I thought that with your reply you were agreeing. Apologies. I don't disagree with anyone's metaphysics. What you do inside your own mind is none of my business. (In my mind, I can still dunk a basketball.) This is a bit of a non sequitur. So what is it that you really disagree with in the analyses performed by myself and others? I have told you many times. Bench test measurements performed over the past 20 years or so prove that it works only in your mind, not in reality. The source impedance of a typical ham transmitter remains somewhat of a mystery during actual operation. The arguments continue to rage after decades of bench test experiments and measurements. The pages of QEX are filled with those arguments. A generator with a 450 Ohm source impedance ... False assumption. That transmitters's source impedance changes away from 450 ohms just as soon as the reflections arrive incident upon the source, i.e. the source impedance is a *variable* that depends upon the magnitude and phase of the reflected wave. If your source impedance is constant, it doesn't match real-world conditions. I think you object to computing the amount of the reverse wave that is reflected at the generator by using the source impedance. I certainly don't object to your computations but the results of those computations have been disproved on the bench using real world ham transmitters over the past 20 years or so. Your simple mental model doesn't correspond to reality unless you take some extraordinary steps which deviate from real-world ham transmitters. Have you taken the time to review those experiments? -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
Jim Kelley wrote:
Hint: people who write physics books know that power does not interfere. Jim, I'll make the same deal with you that I have offered to others with, so far, no takers. If you can prove that I said that powers interfere, I will send you $100. If you cannot prove that, you send me $100, and cease your unfair straw man argument methods. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
On Apr 12, 3:35 am, "Keith Dysart" wrote:
Just for clarity, an example problem that has been previously analysed is the following: A generator with a 450 Ohm source impedance drives a 450 Ohm ideal transmission line terminated in 75 Ohms. What is the magnitude of the re-reflected wave at the generator? Interesting to me that CM railed at me for complaining that his trivial trumped-up non-real-world example wasn't worth considering, and now he's unwilling to accept an example that IS quite realizable. I can EASILY do it on my bench, though I'd prefer to use a 50 ohm generator and 50 ohm line, and a 300 ohm load at the end of the line. It's certainly no more difficult to get a known output source impedance than it is to get a lossless transmission line, but we talk about lossless lines all the time, to remove an unnecessary complication from our discussions. Since we have to test our generators to insure that they really are 50 ohm sources, I feel quite confident that their source impedance doesn't depend on the load you put on them. With respect to the output impedance of a transmitter, it may indeed depend on the tuning/loading of the transmitter's PA, likely even the power level it's running, and _maybe_ even on the load impedance you put on the transmitter's output terminals. But what I do doubt is that it _changes_ for a given setup including a given load impedance, and in steady state, for sure the load impedance isn't changing. So in steady state, can we determine if there are or are not reflections on a transmission line connected to the transmitter, at that interface? If you can't, how much do you have to disturb steady state to make that measurement? If battles have raged on for years about the output source impedance of a transmitter, I submit that the people making the measurements either (a) don't understand what they are doing, or (b) have not fully specified the conditions under which they made the measurement, or both. I assume they would't battle if they agreed they measured different values, but that the conditions were also different, but that may not be a valid assumption--some are known to battle regardless. As I mentioned, we have to be very careful about input and output port impedances in measurement equipment. It's not necessarily an easy thing to get "right," but I'm confident that we've been doing it right, and probably for longer than the "debate" over transmitter output source impedance has been going on. If you don't believe there's a solution to the example Keith posted, you have no right to believe in the results of a measurement with a vector network analyzer, and you should certainly not trust the indicated output level of any signal generator. Cheers, Tom |
Constructive interference in radiowave propagation
On Apr 12, 8:15 am, Cecil Moore wrote:
I have told you many times. Bench test measurements performed over the past 20 years or so prove that it works only in your mind, not in reality. The source impedance of a typical ham transmitter remains somewhat of a mystery during actual operation. The arguments continue to rage after decades of bench test experiments and measurements. The pages of QEX are filled with those arguments. So your only beef with my examples is that they do not accurately model a "typical ham transmitter"? A generator with a 450 Ohm source impedance ... False assumption. That transmitters's source impedance changes away from 450 ohms just as soon as the reflections arrive incident upon the source, i.e. the source impedance is a *variable* that depends upon the magnitude and phase of the reflected wave. When you say that source impedance is a "variable", do you mean this for a "typical ham transmitter", or do you assert that it applies to every generator, even those which can be accurately modelled with a Thevenin equivalent circuit (as many signal generators, even TVSGs can)? I think you object to computing the amount of the reverse wave that is reflected at the generator by using the source impedance. I certainly don't object to your computations but the results of those computations have been disproved on the bench using real world ham transmitters over the past 20 years or so. Which results have been disproved on the bench? Your simple mental model doesn't correspond to reality unless you take some extraordinary steps which deviate from real-world ham transmitters. Have you taken the time to review those experiments? Are the experiments documented in Reflections chapter 19 and 19a representative examples? My read of these chapters is that they offer compelling argument and evidence (at least for the tube style transmitters examined) that ham transmitters are linear*, at least over their normal region of operation. Is it your assertion that these claims are incorrect? ....Keith * Don't confuse this use of linear, which is that the output stage is linear, with whether the input to output transfer function of the transmitter is linear. The transfer function may be non-linear even though the output stage is. |
Constructive interference in radiowave propagation
K7ITM wrote:
If you don't believe there's a solution to the example Keith posted, you have no right to believe in the results of a measurement with a vector network analyzer, and you should certainly not trust the indicated output level of any signal generator. Methinks you have missed the context of the discussion. If the model doesn't work for an IC-706 it is not much use to amateur radio operators. I have already said that a valid model can be had for a signal generator equipped with a circulator load. Now do it for an IC-706. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
On Sun, 08 Apr 2007 20:26:41 GMT, Owen Duffy wrote:
Walter Maxwell wrote in : Walt, I can see that you have taken my comment as personal criticism. That was not intended, and to the extent that I may have caused that, I apologise. In that context, it is better that I refrain from further comment. Regards Owen Hi Owen, Please excuse the long delay in responding to your post of 4-8-07, 4:26 pm EDT. I have been away from the computer since then, attending to personal chores that took priority over rraa. I'm sure your comments weren't meant as a personal attack, and I accept your apology. However, your consideration of statements appearing in Reflections as flawed on the assumption that the concepts presented there concerning impedance matching apply only to lossless and distortionless lines, IMHO is unfair, because it is not true. For readers of your post who now may be questioning the reliability of statements appearing in Reflections, I'm working on a more detailed discussion of the issue for clarification that I will enter on the rraa as a new thread. Walt |
Constructive interference in radiowave propagation
Keith Dysart wrote:
So your only beef with my examples is that they do not accurately model a "typical ham transmitter"? Yes, I have said so about a half-dozen times now. When you say that source impedance is a "variable", do you mean this for a "typical ham transmitter", ... Yes, the discussion is about typical ham transmitters - nothing else matters to typical hams. Which results have been disproved on the bench? Please research the grand argument between Warren Bruene, w5oly, and Walter Maxwell, w2du. Are the experiments documented in Reflections chapter 19 and 19a representative examples? As far as I know, the Bruene/Maxwell argument first saw light in a QST article in the early '90s and has been raging ever since. My read of these chapters is that they offer compelling argument and evidence (at least for the tube style transmitters examined) that ham transmitters are linear*, at least over their normal region of operation. Linear is not the requirement for your source impedance. Constant, fixed, and linear is the requirement for your source impedance. Nothing you have presented had the source impedance as a linear variable. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
Cecil Moore wrote: Jim Kelley wrote: Hint: people who write physics books know that power does not interfere. Jim, I'll make the same deal with you that I have offered to others with, so far, no takers. If you can prove that I said that powers interfere, I will send you $100. If you cannot prove that, you send me $100, and cease your unfair straw man argument methods. Please don't take this the wrong way, Cecil, but after seeing this response to a fairly inert remark, I'm not feeling comfortable enough to take you entirely at your word. Perhaps we just misunderstand each other, but I don't know of another way to interpret what you have written. If you don't believe that power interferes, then why else would you continually write interference equations in terms of power? You can't just arbitrarily throw quantities with any units you like into equations, and then claim authoritative references as your source, Cecil. Is it your contention that interference is not a validating pre-requisite for use in an interference equation? I'm pretty sure somebody using the name Cecil Moore posted Ptot = P1 + P2 +2*SQRT(P1*P2), and used the equation to show how two 100 watt generators generate 400 watts. Help me out. Where did I mess up here? 73, Jim AC6XG |
Constructive interference in radiowave propagation
Jim Kelley wrote:
Perhaps we just misunderstand each other, but I don't know of another way to interpret what you have written. Yes, you do, Jim. You know that I agree with you on almost every technical point yet you incessantly try to erect straw men so you can knock them down. You are almost always trying to discredit someone who agrees with you. To that unfair tactic my response is: From: "An Energy Analysis at an Impedance Discontinuity in an RF Transmission Line", by W5DXP, WorldRadio, Oct. 2005 "Single-source RF energy in a transmission line and laser light are both coherent electromagnetic energy waves that obey the laws of superposition, interference, conservation of energy, and conservation of momentum." "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. Any sign associated with a power in this paper is the sign of the cosine of the phase angle between two voltage phasors." If you don't believe that power interferes, then why else would you continually write interference equations in terms of power? Because that's what Dr. Best, Hecht, and Born and Wolf do. Intensity, irradiance, and Poynting vectors are *power* densities. Multiply the following intensity-irradiance equation by unit-area and what do you get? Why, you get WATTS of power! Itot = I1 + I2 + 2*SQRT(I1*I2)cos(A) in watts/unit-area Multiplying both sides of the equation by unit-area Ptot = P1 + P2 + 2*SQRT(P1*P2)cos(A) in watts I assume that's how Dr. Best came up with the equation. Or don't even multiply by unit area - just use Poynting vectors instead where each P above is a Poynting vector. The dimensions of a Poynting vector are identical to the dimensions of irradiance and intensity. You can't just arbitrarily throw quantities with any units you like into equations, and then claim authoritative references as your source, Cecil. I have not done that, Jim. The Poynting vector has exactly the same units as intensity and irradiance. Multiply both sides of the equation by unit-area and the result is WATTS, the unit of power and that's fully consistent with the rules of mathematics. Is it your contention that interference is not a validating pre-requisite for use in an interference equation? The question appears to have a trivial answer so it must be just another straw man. Yes, interference exists if interference exists and interference doesn't exist if interference doesn't exist. Satisfied? I'm pretty sure somebody using the name Cecil Moore posted Ptot = P1 + P2 +2*SQRT(P1*P2), and used the equation to show how two 100 watt generators generate 400 watts. Help me out. Where did I mess up here? False so just another straw man. I said two 100 watt generators do *NOT* generate 400 watts because there is no interference between the generators. Maybe you need your glasses changed? I did follow that posting up showing how two 100 watt *waves* can engage in total constructive interference and obtain a total of 400 watts. Even you should be able to figure out how two 100 watt generators can be made to produce a forward power of 400 watts in a transmission line with an SWR of 5.83:1 and that is perfectly consistent with Hecht, and Born & Wolf's intensity equations. ************************************************** **************** HECHT AND BORN & WOLF'S TOTAL CONSTRUCTIVE INTERFERENCE EQUATIONS ASSUME THERE IS AN EQUAL MAGNITUDE OF TOTAL DESTRUCTIVE INTERFERENCE OCCURRING SOMEWHERE ELSE TO SATISFY THE REQUIREMENTS OF THE CONSERVATION OF ENERGY PRINCIPLE. For every total constructive interference equation I1 + I2 + 2*SQRT(I1*I2), there exists a total destructive interference equation I1 + I2 - 2*SQRT(I1*I2) The destructive interference and constructive interference always sum to a net power density of ZERO such that the AVERAGE power always remains the same. ************************************************** **************** Let's say we have two light waves of 100 watts/cm^2 intensity and we cause them to interfere constructively. Here's the intensity equation for total constructive interference. I1 + I2 + 2*SQRT(I1*I2) = 100 + 100 + 2*SQRT(100*100) = 400 watts/cm^2 Multiply both sides of the equation by cm^2 and you get 400 watts of power and indeed that square cm would be getting very warm. Somewhere else exists a square cm with zero intensity. That is Born and Wolf's equation (16a) on page 259 of the 4th edition of "Principles of Optics). The equation is correct and the dimensions are correct. It is also Hecht's equation (9.15) on page 388 of the 4th edition of "Optics". Those authors all label the 2*SQRT(I1*I2) term as the *interference term*. Let's say we have two RF waves or 100 watts/cm^2 intensity and we cause them to interfere constructively in a coax transmission line with a cross sectional area of one square cm. P1 + P2 + 2*SQRT(P1*P2) = 100 + 100 + 2*SQRT(100*100) = 400 watts/cm^2. With those dimensions, the intensity equation and the Poynting vector equation are EXACTLY the same. This is equation 12 from Dr. Best's QEX article, "Wave Mechanics of Transmission Lines, Part 3: ..." in the Nov/Dec 2001 edition. The fixed cross sectional area of the coax is redundant and we can choose to deal entirely with watts. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
Jim Kelley wrote:
I'm pretty sure somebody using the name Cecil Moore posted Ptot = P1 + P2 +2*SQRT(P1*P2), and used the equation to show how two 100 watt generators generate 400 watts. Help me out. Where did I mess up here? Jim, you asked me not to tell you what you said but instead to furnish the quote showing what you said. Above you are violating the rules you asked me to abide by. Produce that quote and I will explain it. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
On Apr 12, 3:23 pm, Cecil Moore wrote:
K7ITM wrote: If you don't believe there's a solution to the example Keith posted, you have no right to believe in the results of a measurement with a vector network analyzer, and you should certainly not trust the indicated output level of any signal generator. Methinks you have missed the context of the discussion. If the model doesn't work for an IC-706 it is not much use to amateur radio operators. I have already said that a valid model can be had for a signal generator equipped with a circulator load. The only problem with this statement is the assumption that the result can only be achieved with a circulator. It only takes a 10 cent resistor. You really should put down your optics books for a few hours and crack open a basic circuit theory or transmission line text. Or google, "'lattice diagrams' reflection". For matching at the source, only 10 cent resistors are used. ....Keith |
Constructive interference in radiowave propagation
On Apr 12, 3:37 pm, Cecil Moore wrote:
Keith Dysart wrote: So your only beef with my examples is that they do not accurately model a "typical ham transmitter"? Yes, I have said so about a half-dozen times now. When you say that source impedance is a "variable", do you mean this for a "typical ham transmitter", ... Yes, the discussion is about typical ham transmitters - nothing else matters to typical hams. So when a poster presents a problem in a context other "typical ham transmitters", why do you dispute the answers. If you can't discuss the problem in the context presented by the poster, why not have the courtesy to stay out. Others may be interested in learning about how things relate in contexts other than "typical ham transmitters". Why sabotage the discussions by arguing and arguing and then saying "Oh, I only meant my comments in the context of "typical ham transmitters" WHICH WAS NOT THE CONTEXT OF THE PROBLEM STATEMENT. And kindly stop using the Texas A&M example of TVSG and 1000 feet of line. It is clearly out of your context of "typical ham transmitters". Perhaps, in your dissertations on optics, it would be valuable to state that they apply only in the context of "typical ham transmitters". This might make it clear to the reader that your suggestions are not generally applicable and could reduce the wasted bits. Which results have been disproved on the bench? Please research the grand argument between Warren Bruene, w5oly, and Walter Maxwell, w2du. Are the experiments documented in Reflections chapter 19 and 19a representative examples? As far as I know, the Bruene/Maxwell argument first saw light in a QST article in the early '90s and has been raging ever since. My read of these chapters is that they offer compelling argument and evidence (at least for the tube style transmitters examined) that ham transmitters are linear*, at least over their normal region of operation. Linear is not the requirement for your source impedance. Constant, fixed, and linear is the requirement for your source impedance. Nothing you have presented had the source impedance as a linear variable. No indeed, the source impedance was a constant and resistive in all my examples. That meets the needs for linear analysis. Remember f(a+b) = f(a) + f(b)? You are claiming that for "typical ham transmitters" the source impedance is undefinable. This is quite at odds with the exposition in Reflections chapters 19 and 19a. Or maybe not, after all, Reflections is quite precise and claims only for a specific class of ham transmitters, which, I suppose, may not be typical. Though they look so to me. So I take it that you no longer agree with the analysis presented in Reflections 19 and 19a. I am pretty sure that you have stated agreement in the past. It would be valuable if you were to expand on the reasons for your change of thought. What convinced you that "typical ham transmitters" could not have their source impedance measured? ....Keith |
Constructive interference in radiowave propagation
Owen Duffy wrote:
Cecil, you have conveniently clipped the context (as you do), the relevant context being the line-load interface and source-line interface. Following published usenet rules, I trim the part to which I am not replying. 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). Those statements are generally about lossless lines where the Z0 is purely resistive. In the lossless wave reflection model, there is no reactive energy in the transmission line. The forward voltage is in phase with the forward current and the reflected voltage is 180 degrees out of phase with the reflected current. Both V*I*cos(theta) terms are in watts with zero vars. Of course, real world transmission lines have (hopefully negligible) vars. 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. It is NOT the distributed impedance model to which I object. It is the lumped circuit model which assumes the speed of light is infinite and 75m loading coils don't occupy any space. Here's a quote from an IEEE white paper at: http://www.ttr.com/TELSIKS2001-MASTER-1.pdf "Consequently, lumped element circuit theory does not (and cannot) accurately embody a world of second order partial differential equations in space and time." -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
Keith Dysart wrote:
The only problem with this statement is the assumption that the result can only be achieved with a circulator. Please stop putting words into my mouth. I said it could be achieved with a circulator. I did *NOT* say it could *only* be achieved with a circulator. It only takes a 10 cent resistor. That is naive in the extreme and makes you sound about ten years old. If a 10 cent resistor would accomplish that in the real world, nobody would ever buy a circulator. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
On Apr 12, 8:06 pm, Cecil Moore wrote:
Owen Duffy wrote: Cecil, you have conveniently clipped the context (as you do), the relevant context being the line-load interface and source-line interface. Following published usenet rules, I trim the part to which I am not replying. 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). Those statements are generally about lossless lines where the Z0 is purely resistive. In the lossless wave reflection model, there is no reactive energy in the transmission line. The forward voltage is in phase with the forward current and the reflected voltage is 180 degrees out of phase with the reflected current. Both V*I*cos(theta) terms are in watts with zero vars. Of course, real world transmission lines have (hopefully negligible) vars. There are two models that can accurately describe the same phenomenon: the power folk like VAs, Watts and VARs; the RF folk like forward and reverse travelling waves. But the phenomenon is the same. One can indeed describe what happens on a transmission line in terms of VAs, Watts, and VARs and any line that has a reverse wave will be found to have VARs. The different terms apply to different models, not to different situations. Just another reason why you have to be careful when you think that the forward and reverse waves necessarily represent real power. Trust the power folk on this one; they know what represents real power, they are billing for it. And its Watts. Net. They only power that counts is the power you can bill for. ....Keith |
Constructive interference in radiowave propagation
Keith Dysart wrote:
So when a poster presents a problem in a context other "typical ham transmitters", why do you dispute the answers. Uhhhhhh Keith, because you presented the problem to me, not someone else. You asked me what was wrong with your examples. I obliged you. If you don't want me to answer, don't ask me to respond. Perhaps, in your dissertations on optics, it would be valuable to state that they apply only in the context of "typical ham transmitters". This might make it clear to the reader that your suggestions are not generally applicable and could reduce the wasted bits. Perhaps, you should learn to recognize the common misleading logical diversions, including your reductio ad absurdum assertion above, and avoid them in the future. No indeed, the source impedance was a constant and resistive in all my examples. Did you bench test it or just dream it up and wave your hands? Maybe your ten cent resistor can resolve the war in Iraq - in your mind. So I take it that you no longer agree with the analysis presented in Reflections 19 and 19a. I am pretty sure that you have stated agreement in the past. Please stop putting words in my mouth. I have never stated agreement or disagreement. It is just one possibility out of many that have been presented over the years. The fact that there are so many theories is proof that it has not been settled. Why don't you whip out an article that settles everything and see what QEX thinks about it? It would be valuable if you were to expand on the reasons for your change of thought. Since I haven't changed my thought, that would be difficult. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
Keith Dysart wrote:
Just another reason why you have to be careful when you think that the forward and reverse waves necessarily represent real power. Trust the power folk on this one; they know what represents real power, they are billing for it. And its Watts. Net. They only power that counts is the power you can bill for. :-) :-) :-) Uhhhhhh Keith, the power company does NOT bill you for "Watts. Net." They bill you for the number of joules (KWH) that you convert from 60 Hz AC to heat. Where the heck did you learn your physics? Last month I converted 3,452,400,000 joules to heat here at my QTH. That's 0.000002442 cents per joule. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
On Apr 12, 8:20 pm, Cecil Moore wrote:
Keith Dysart wrote: The only problem with this statement is the assumption that the result can only be achieved with a circulator. Please stop putting words into my mouth. I said it could be achieved with a circulator. I did *NOT* say it could *only* be achieved with a circulator. Do you have a list of possible approaches? Is there any environment in which a 10 cent resistor is the optimal solution? It only takes a 10 cent resistor. That is naive in the extreme and makes you sound about ten years old. If a 10 cent resistor would accomplish that in the real world, nobody would ever buy a circulator. In my world, the solution is optimized for the problem at hand: sometimes a circulator, sometimes a resistor, sometimes feedback and sometimes we just don't care about matching the source so nothing at all is needed. ....Keith |
Constructive interference in radiowave propagation
Keith Dysart wrote:
Do you have a list of possible approaches? I only use one - I don't allow reflected energy to become incident upon my IC-706 and IC-756PRO. That is, by far, the most common configuration in amateur radio. Is there any environment in which a 10 cent resistor is the optimal solution? To the best of my knowledge, not on the output of any 100 watt amateur radio transmitter. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
"Keith Dysart" wrote in
ups.com: .... Just another reason why you have to be careful when you think that the forward and reverse waves necessarily represent real power. Trust the power folk on this one; they know what represents Keith, that was indeed my point, that talking of the forward and reflected waves as power waves (or whatever non-phasor term is being used today) and the assertion that those "power" waves are entirely real power (for whatever reasons), and the talk of superposition of these waves (where the examples seem to deal with power algebraicly with sometimes a fudge for phase correction) cannot explain the role of a transmission line as an energy store at any instant, nor the exchange of reactive energy at source and load over time. If that seems a jumble, it is because this stuff is bandied around without much discipline. In the same vein, I saw an assertion without sufficient qualification that in a transmission line, 50% of the energy is stored / contained in the electric field and 50% in the magnetic field. Again, general statements from specific cases. It isn't the special case of a lossless line the causes this, it is the conclusions that are incorrectly drawn from the lossless line or incorrectly applied that are the problem. Owen |
Constructive interference in radiowave propagation
Owen Duffy wrote:
Keith, that was indeed my point, that talking of the forward and reflected waves as power waves ... If you are trying to quote me, Owen, you are misquoting me. Exactly what is it about the following excerpts from my 2005 energy article with which you disagree? From: "An Energy Analysis at an Impedance Discontinuity in an RF Transmission Line", by W5DXP, WorldRadio, Oct. 2005 "Single-source RF energy in a transmission line and laser light are both coherent electromagnetic energy waves that obey the laws of superposition, interference, conservation of energy, and conservation of momentum." "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." -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
On Apr 12, 4:50 pm, "Keith Dysart" wrote:
On Apr 12, 3:23 pm, Cecil Moore wrote: K7ITM wrote: If you don't believe there's a solution to the example Keith posted, you have no right to believe in the results of a measurement with a vector network analyzer, and you should certainly not trust the indicated output level of any signal generator. Methinks you have missed the context of the discussion. If the model doesn't work for an IC-706 it is not much use to amateur radio operators. I have already said that a valid model can be had for a signal generator equipped with a circulator load. The only problem with this statement is the assumption that the result can only be achieved with a circulator. It only takes a 10 cent resistor. You really should put down your optics books for a few hours and crack open a basic circuit theory or transmission line text. Or google, "'lattice diagrams' reflection". For matching at the source, only 10 cent resistors are used. ...Keith Well, I'm not sure that's the ONLY problem with it, Keith! ;-) Whether the model works for me with an IC-706 will have to wait till someone sends me an operating IC-706 to test. (They should not expect its return...) But I can assure you that whether it does or not, it's a VERY useful model to me, and I am an amateur radio operator. I certainly do NOT accept that the context of this thread is amateur transmitters--there's been so much basenote drift by this time that practically anything relating to vector addition of signals seems fair game. Cheers, Tom PS--know any circulators that work over a range from 10kHz to 6GHz?? Know any that work at 10kHz even? |
Constructive interference in radiowave propagation
Owen Duffy wrote:
"In the same vein, I saw an assertion without sufficient qualification that in a transmission line, 50% of the energy is stored/contained in the electric field and 50% in the magnetic field. Again, general statements from specified cases." Now we accept that energy travels a guided path as an EM wave. The electric and magnetic fields of a wave alternately contain the energy of the wave. When the electric-field is at its maximum, the magnetic-field is at its minimum, and vice versa. The change in one field induces the other field and vice versa. Thus it is the same energy which is being passed back and forth between both fields. Therefore, over a prolonged period, 50% resides in each field. Best regards, Richard Harrison, KB5WZI |
Constructive interference in radiowave propagation
K7ITM wrote:
I certainly do NOT accept that the context of this thread is amateur transmitters-- Granted, the thread drifted away from the subject line which has little to do with transmitters, but amateur transmitters are what the entire Maxwell-Bruene brouhaha is all about. We already have a special case where a signal generator plus circulator yields everything we need to know. One more special case doesn't add much even if it works which is questionable. We do not have a valid generalized case that covers amateur radio transmitters. IMO, that's what the brouhaha is all about. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
Richard Harrison wrote:
Owen Duffy wrote: "In the same vein, I saw an assertion without sufficient qualification that in a transmission line, 50% of the energy is stored/contained in the electric field and 50% in the magnetic field. Again, general statements from specified cases." Now we accept that energy travels a guided path as an EM wave. The electric and magnetic fields of a wave alternately contain the energy of the wave. When the electric-field is at its maximum, the magnetic-field is at its minimum, and vice versa. In addition: Assuming ideal TEM waves, the B-field (magnetic) is always orthogonal to the E-field (electric) and both are orthogonal to the direction of travel. The power associated with the ideal TEM wave is ExB in watts (no vars). A TEM wave travels at the c' = c(VF) speed of light and cannot travel at any other speed. If it slows down or stops, it is not longer a TEM wave and has necessarily been converted to some other form of energy. Energy "sloshing" back and forth between reactances is NOT TEM energy. The principle of superposition gives us permission to treat the forward traveling wave and reverse traveling wave separately and superpose the results. Superposing the results does NOT change the nature of the TEM waves. The fact that the net total fields are no longer orthogonal gives the illusion that there exist vars in the circuit but they are only virtual vars based on virtual voltages and virtual currents. There are no vars in ideal TEM waves in ideal lossless purely resistive Z0 transmission lines. The forward traveling wave TEM fields have no effect on the reverse traveling wave TEM fields as long as a physical impedance discontinuity is not encountered. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
On Sun, 08 Apr 2007 20:26:41 GMT, Owen Duffy wrote:
Owen, the following is a copy of your post of 4-8-07, and my response 0n 4-12-07 to which you haven't responded. Perhaps you haven't seen my response, or perhaps you chose not to respond, which is ok either way. Walter Maxwell wrote in : Walt, I can see that you have taken my comment as personal criticism. That was not intended, and to the extent that I may have caused that, I apologise. In that context, it is better that I refrain from further comment. Regards Owen Hi Owen, Please excuse the long delay in responding to your post of 4-8-07, 4:26 pm EDT. I have been away from the computer since then, attending to personal chores that took priority over rraa. I'm sure your comments weren't meant as a personal attack, and I accept your apology. However, your consideration of statements appearing in Reflections as flawed on the assumption that the concepts presented there concerning impedance matching apply only to lossless and distortionless lines, IMHO is unfair, because it is not true. For readers of your post who now may be questioning the reliability of statements appearing in Reflections, I'm working on a more detailed discussion of the issue for clarification that I will enter on the rraa as a new thread. Walt |
Constructive interference in radiowave propagation
Owen Duffy wrote:
"Richard "over a prolonged period" is a qualification, and still doesn`t sufficiently qualify the statement to be true." Maybe not the best words, but they are true in the practical case. In an EM-wave, energy is being passed back and forth netween the electric and magnetic fields on a periodic basis. At any given instant most of the wave`s energy may reside mostly in one field or the other at a given point. Half a cycle nas no practical significance among a million or more. Best regards, Richard Harrison, KB5WZI |
Constructive interference in radiowave propagation
Walter Maxwell wrote:
On Sun, 08 Apr 2007 20:26:41 GMT, Owen Duffy wrote: Owen, the following is a copy of your post of 4-8-07, and my response 0n 4-12-07 to which you haven't responded. Perhaps you haven't seen my response, or perhaps you chose not to respond, which is ok either way. Perhaps instead of asking Owen to point out what is wrong with your writings, he would be more comfortable discussing his theory, given the Vr and Ir terms that he uses, of how the energy associated with that Vr and Ir wave gets its direction and momentum changed at a Z0-match when Vr and Ir are canceled/re-reflected/redistributed. -- 73, Cecil, w5dxp.com |
Constructive interference in radiowave propagation
Owen Duffy wrote:
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. Given that the S-Parameter analysis is valid as explained in HP's Ap Note 95-1 available from: http://www.tm.agilent.com/data/stati...-1/an-95-1.pdf --------Z01--------+--------Z02-------- a1-- b2-- --b1 --a2 where a1, a2, b1, and b2 are normalized voltages. The equation for b1 is b1 = s11(a1) + s12(a2) Given that a1 and a2 are in phase and that b1 = 0 then s11(a1) and s12(a2) would have to be of equal magnitude and opposite phase thus making the reflected power |b1|^2 equal to zero. s11(a1) and s12(a2) cancel each other out. (What happens to the energy in the canceled waves?) What do you get when you square both sides of the equation:? b1 = s11(a1) + s12(a2) = 0 reflected voltage Since the square of any of those terms yields watts, If we simplify by replacing complicated terms with symbols: |s11*a1|^2 = P1 and |s12*a2|^2 = P2 we get: |b1|^2 = 0 = P1 + P2 - 2*SQRT(P1*P2) = 0 reflected power These squared (power) terms are all explained in Ap Note 95-1. The intensity-irradiance-Poynting vector equation can be derived from the S-Parameter equations. Good thing the S-Parameter analysis is consistent with Hecht and Born & Wolf, huh? -- 73, Cecil, w5dxp.com |
Constructive interference in radiowave propagation
Cecil Moore wrote: Perhaps instead of asking Owen to point out what is wrong with your writings, he would be more comfortable discussing his theory, given the Vr and Ir terms that he uses, of how the energy associated with that Vr and Ir wave gets its direction and momentum changed at a Z0-match when Vr and Ir are canceled/re-reflected/redistributed. -- 73, Cecil, w5dxp.com You seem to be implying that there's something different about how these electromagnetic waves change direction compared to other electromagnetic waves. Why is that? 73, ac6xg |
Constructive interference in radiowave propagation
Cecil Moore wrote: "Powers, treated as scalars, are incapable of interference." And when powers sic are not treated as scalers, then sometimes it's ok to use power in interference equations, but other times it's not - pretty much just depending on whether or not you get the answer you want. And sometimes you have to either add or subtract the amount of power that isn't somewhere else, or else average with zero in order to get the right answer. All this and more, this week on r.r.a.a. :-) AC6XG |
Constructive interference in radiowave propagation
Jim Kelley wrote:
You seem to be implying that there's something different about how these electromagnetic waves change direction compared to other electromagnetic waves. Why is that? There is something different but not unusual. We don't often observe wave cancellation of visible light waves because of the problem of getting coherent beams of light perfectly aligned. Yet, we experience RF wave cancellation every time we adjust our antenna tuners for a Z0-match because the perfect alignment of coherent RF waves inside a piece of coax is an automatic given. Here's a very simple example. The measured forward and reflected powers are given. The source and load impedances are irrelevant and the length of the Z01 and Z02 lines are irrelevant. Any one of these measured values could be unknown and solved for by calculations based on the conservation of energy principle. ------Z01------+------Z02------ Pfor1=100w-- Pfor2=200w-- --Pref1=0w --Pref2=100w We have 100 joules/sec incident upon the Z0-match point from the direction of the source. We have 100 joules/sec incident upon the Z0-match point from the direction of the load. Those waves combine to obtain 200 joules/sec toward the load. It is obvious that Pref2 has to change direction and momentum for that condition to exist. The power reflection coefficient, rho^2, is obviously 0.5 so the voltage reflection coefficient, rho, is just as obviously +/- 0.707, depending upon whether [Z02 Z01] or [Z02 Z01}. The direction and momentum of the Pref2 reflected wave obviously reverses at the Z0-match point '+'. Exactly how does the direction and momentum of the Pref2 wave get reversed? Where are the physics equations for that process that we hams label "re-reflection"? You and others have been strangely silent on that subject preferring to kibitz rather than provide any technical insight. An exact duplicate of the above conditions would exist with a 100w laser beam traveling through 1/2WL of thin film with an index of refraction of 5.83. A B i=1.0 | i=5.83 | i=1.0 100w laser---air---|--1/2WL thin-film--|---air---... --Pref1=0w | --Pref2=100w | --Pref3=0w Pfor1=100w | Pfor2=200w-- | Pfor3=100w-- What happens to reverse the direction and momentum of the internal reflection in the thin film? Hint: Both Hecht and Born & Wolf give the equations for what happens at plane A. And yes, the S-Parameter equations agree 100% with them. -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
Jim Kelley wrote:
Cecil Moore wrote: "Powers, treated as scalars, are incapable of interference." And when powers sic are not treated as scalers, ... There you go again, Jim, trying to set up a straw man. I do NOT treat powers as anything except scalars. Any phase angle that enters into the calculation is the phase angle between the two voltages associated with those powers. They are copied directly from Hecht, Born & Wolf, and the S-Parameter analysis. Why not, instead of your underhanded, unethical kibitzing, present your own set of equations that govern the process that we hams call "re-reflection"? -- 73, Cecil http://www.w5dxp.com |
Constructive interference in radiowave propagation
Cecil Moore wrote: What happens to reverse the direction and momentum of the internal reflection in the thin film? That's what I was asking you. You seem to be hinting at something, but not actually saying it. What, other than reflection, are you suggesting causes electromagnetic waves to reverse their direction of propagation in the system you describe? Thank you, AC6XG |
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