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Analyzing Stub Matching with Reflection Coefficients
Gene Fuller wrote:
Cecil Moore wrote: This is steady-state after the wave interaction. What you guys don't seem to realize is that s11(a1) and s12(a2) are continually changing, continually interacting, and a1 & a2 are rotating phasors changing with time. Utter nonsense. Any setup that includes t0 or t=0 is not steady state. Gene, you obviously misunderstood what I said. There is no t0 or t=0 in my above statement. It is just that the delta-t doesn't change from the transient state to the steady-state. In an s-parameter analysis: The normalized voltage, a1, equals Vi1/SQRT(Z0) where 'i' stands for incident voltage. a2 equals Vi2/SQRT(Z0). These voltages are normally represented in phasor notation but they can just as easily be represented in exponential notation where a1 = Vi1*e^jwt+X and a2 = Vi2*e^jwt+Y, where X and Y are constant phase angles. Thus, the s-parameter equation becomes: b1 = Vi1[cos(wt+X)]/SQRT(Z0) + Vi2[cos(wt+Y)]/SQRT(Z0) = 0 adding the delta-t "tick" gives: b1 = Vi1{cos[w(t+delta-t)+X]}/SQRT(Z0) + Vi2{cos[w(t+delta-t)+Y]}/SQRT(Z0) = 0 Vi1 obviously has to be an equal magnitude to Vi2 and X and Y obviously have to be 180 degrees apart. Given that, for every delta-t "tick" of time, the two real normalized voltages sum to zero. The square of the normalized RMS value gives average power in each wave. The equation can be turned into a differential equation by having delta-t approach zero in the limit. -- 73, Cecil http://www.w5dxp.com |
Analyzing Stub Matching with Reflection Coefficients
Keith Dysart wrote:
You really do need to realize that there is no need for a circulator. So Tektronix can just abandon its circulator business and kiss their circulator profits goodbye? When are you going to patent your idea and get rich? There you go. Still stuck. You really should crack the books in search of a reference to support your contention. You won't find one. And that is exactly why the argument has been raging for decades. Humans have not yet acquired 100% of all knowledge. You seem to claim that you have mastered that task but I seriously doubt it. And the relevence of the conjugate match is that the conjugate is the generator source impedance and it is the impedance that the wave incident upon the generator sees. I see you have not yet read Walter Maxwell's article. The generator source impedance is not what is seen by the reflected waves. I have certainly never said that. If you could point me to the words that misled you into thinking that, I will attempt to clarify your misunderstanding. Correct me if I'm wrong. I understood you to say that energy cannot flow past an instantaneous zero energy point yet there is an instantaneous zero energy point every 1/2WL in an EM traveling wave. -- 73, Cecil http://www.w5dxp.com |
Analyzing Stub Matching with Reflection Coefficients
Keith Dysart wrote:
On Apr 20, 12:46 pm, Cecil Moore wrote: I already did - Bruene's early 1990's QST article. Sorry. Not a good enough description for any kind of analysis. Ignore it if you choose. That's when the present hoopla began, at least in the amateur radio community. You can follow the thread from that point to the present to see what is happening in the present. Nothing to sweep under the rug, I am afraid. It is key that the dissipation depends on the design of the generator. Some times those 'reverse watts' cause the dissipation to drop to 0, sometimes they cause it to increase by a factor of 4, sometimes they cause it to increase by the numerical value of the 'reverse watts'. Pretty much hard to argue that those 'reverse watts' are real when their heating effect is so variable. Not at all. The heating effect depends upon how much of the reverse joules/sec are re-reflected. If the dissipation drops to 0, that is prima facie evidence that all the reflected joules/sec have been re-reflected. If the dissipation increases by a factor of 4, that is prima facie evidence that all of the reflected joules/sec are being dissipated in the source along with all of the joules/sec available from the source into a matched load. Anything else would violate the conservation of energy principle. I'd suggest you think of power as a quantity not a situation. Superposition works for linear, time invariant circuits with multiple sources. Check any text book. The generators and lines under discussion meet these requirements. But superposition obviously doesn't work at the source *point*. One possible technical conclusion may be that the dynamic active source is constant, fixed, and refuses to be superposed (for any constant, fixed load). If that is true, it would certainly stop the present raging debate in its tracks. -- 73, Cecil http://www.w5dxp.com |
Analyzing Stub Matching with Reflection Coefficients
Cecil Moore wrote:
Gene Fuller wrote: Cecil Moore wrote: This is steady-state after the wave interaction. What you guys don't seem to realize is that s11(a1) and s12(a2) are continually changing, continually interacting, and a1 & a2 are rotating phasors changing with time. Utter nonsense. Any setup that includes t0 or t=0 is not steady state. Gene, you obviously misunderstood what I said. There is no t0 or t=0 in my above statement. It is just that the delta-t doesn't change from the transient state to the steady-state. In an s-parameter analysis: The normalized voltage, a1, equals Vi1/SQRT(Z0) where 'i' stands for incident voltage. a2 equals Vi2/SQRT(Z0). These voltages are normally represented in phasor notation but they can just as easily be represented in exponential notation where a1 = Vi1*e^jwt+X and a2 = Vi2*e^jwt+Y, where X and Y are constant phase angles. Thus, the s-parameter equation becomes: b1 = Vi1[cos(wt+X)]/SQRT(Z0) + Vi2[cos(wt+Y)]/SQRT(Z0) = 0 adding the delta-t "tick" gives: b1 = Vi1{cos[w(t+delta-t)+X]}/SQRT(Z0) + Vi2{cos[w(t+delta-t)+Y]}/SQRT(Z0) = 0 Vi1 obviously has to be an equal magnitude to Vi2 and X and Y obviously have to be 180 degrees apart. Given that, for every delta-t "tick" of time, the two real normalized voltages sum to zero. The square of the normalized RMS value gives average power in each wave. The equation can be turned into a differential equation by having delta-t approach zero in the limit. Cecil, I should have know better than to read this with a cup of coffee in my hand. I just snorted coffee all over my keyboard. 8-) 73, Gene W4SZ |
Analyzing Stub Matching with Reflection Coefficients
Gene Fuller wrote:
I should have know better than to read this with a cup of coffee in my hand. I just snorted coffee all over my keyboard. Your highly technical rebuttal of my posting is noted. Have you ever seen the equation? The integral of e to the x = function of u to the n __ |_ __|e^x = F(u^n) -- 73, Cecil http://www.w5dxp.com |
Analyzing Stub Matching with Reflection Coefficients
Gene Fuller wrote:
I should have know better than to read this with a cup of coffee in my hand. I just snorted coffee all over my keyboard. Gene, I've got an experiment for you. Go to: http://micro.magnet.fsu.edu/primer/j...ons/index.html and set one phase to 0 and the other phase to 180 degrees. Then get an index card and cover up everything to the left except one point on each wave. All you see is those two single points moving up and down. That gives you a visual idea of how s11(a1) and s12(a2) originate and are canceled at a Z0-match *point*. Plot those points back in time and you will have a history of the canceled waves from which you can compute average power density as |s11(a1)|^2 and |s12(a2|^2. -- 73, Cecil http://www.w5dxp.com |
Analyzing Stub Matching with Reflection Coefficients
Cecil Moore wrote:
Gene Fuller wrote: I should have know better than to read this with a cup of coffee in my hand. I just snorted coffee all over my keyboard. Gene, I've got an experiment for you. Go to: http://micro.magnet.fsu.edu/primer/j...ons/index.html and set one phase to 0 and the other phase to 180 degrees. Then get an index card and cover up everything to the left except one point on each wave. All you see is those two single points moving up and down. That gives you a visual idea of how s11(a1) and s12(a2) originate and are canceled at a Z0-match *point*. Plot those points back in time and you will have a history of the canceled waves from which you can compute average power density as |s11(a1)|^2 and |s12(a2|^2. Cecil, You are going to pull a brain muscle by stretching so much. Are you suggesting that two wiggling points on a web page are the key to understanding the universe? Here's a thought experiment for you. Read the message by Tom, K7ITM, where he copied a quote from physicsforums.com. See if you can figure out how those waves you insist are created and then quickly canceled (delta-t later) might have never existed in the first place. Hint: waves don't interact with each other, but they do interact with materials containing electrons. (I believe that covers quite a few materials.) 73, Gene W4SZ |
Analyzing Stub Matching with Reflection Coefficients
On Apr 21, 8:35 am, Cecil Moore wrote:
Keith Dysart wrote: I have certainly never said that. If you could point me to the words that misled you into thinking that, I will attempt to clarify your misunderstanding. Correct me if I'm wrong. I understood you to say that energy cannot flow past an instantaneous zero energy point yet there is an instantaneous zero energy point every 1/2WL in an EM traveling wave. Actually I said a zero power point, but you are essentially correct. If the zero power point is stationary then no energy can be flowing. When energy is flowing, either there is no zero power point, or the zero power point is moving as well. At a given point on the line, when the voltage or current is always zero then no energy is flowing. When energy is flowing, the voltage and current will not always be zero at that point. There can also be a voltage and current but they can be 90 degrees out of phase so no net energy flows. In this case, energy will flow first forward then backwards with an average of zero. ....Keith |
Analyzing Stub Matching with Reflection Coefficients
On Apr 21, 8:47 am, Cecil Moore wrote:
Keith Dysart wrote: Nothing to sweep under the rug, I am afraid. It is key that the dissipation depends on the design of the generator. Some times those 'reverse watts' cause the dissipation to drop to 0, sometimes they cause it to increase by a factor of 4, sometimes they cause it to increase by the numerical value of the 'reverse watts'. Pretty much hard to argue that those 'reverse watts' are real when their heating effect is so variable. Not at all. The heating effect depends upon how much of the reverse joules/sec are re-reflected. If the dissipation drops to 0, that is prima facie evidence that all the reflected joules/sec have been re-reflected. If the dissipation increases by a factor of 4, that is prima facie evidence that all of the reflected joules/sec are being dissipated in the source along with all of the joules/sec available from the source into a matched load. Anything else would violate the conservation of energy principle. So you expect that some of the reverse wave is reflected at the generator and yet experiment has shown that none of the reverse wave is reflected at the generator when the generator] source impedance is the same as the line characteristic impedance. I am curious as to why you ignore these experimental results. I'd suggest you think of power as a quantity not a situation. Superposition works for linear, time invariant circuits with multiple sources. Check any text book. The generators and lines under discussion meet these requirements. But superposition obviously doesn't work at the source *point*. One possible technical conclusion may be that the dynamic active source is constant, fixed, and refuses to be superposed (for any constant, fixed load). If that is true, it would certainly stop the present raging debate in its tracks. As you noted previously, it does not matter whether the reverse wave is created by a reflection or another generator. So the experiment has been done with a generator at both ends of the line and the results are entirely consistent with the results predicted using the generator source impedance to compute the amount of reflection. I am curious as to why you ignore these results. And, of course, there results are consistent with the analysis described in any basic text book on transmission lines. ....Keith |
Analyzing Stub Matching with Reflection Coefficients
Gene Fuller wrote:
You are going to pull a brain muscle by stretching so much. Are you suggesting that two wiggling points on a web page are the key to understanding the universe? No, just wave cancellation. If the graphic is completely incorrect, as you say, why did they publish it? -- 73, Cecil http://www.w5dxp.com |
Analyzing Stub Matching with Reflection Coefficients
Keith Dysart wrote:
If the zero power point is stationary then no energy can be flowing. Time for you to review EM waves, Keith. There is a zero power point in every EM traveling wave every 1/2WL where the E-field and H-field are both zero at the same time. -- 73, Cecil http://www.w5dxp.com |
Analyzing Stub Matching with Reflection Coefficients
Keith Dysart wrote:
So you expect that some of the reverse wave is reflected at the generator and yet experiment has shown that none of the reverse wave is reflected at the generator when the generator] source impedance is the same as the line characteristic impedance. I am curious as to why you ignore these experimental results. Those "experimental results" paper-only results are a figment of your imagination. You zero energy level source proved just the opposite. -- 73, Cecil http://www.w5dxp.com |
Analyzing Stub Matching with Reflection Coefficients
On Apr 20, 5:34 pm, Cecil Moore wrote:
Jim Kelley wrote: There is no support for your claim. There is plenty of support for my claim, Jim, but you deleted it. I will simply repost it over and over until you respond. Given the following experiment with two signal generators equipped with circulators and load resistors - the generators are phased-locked to ensure coherency. The two feedlines are of equal electrical lengths. SGCL1 is turned on. SGCL2 is turned off. 100W | 25W 50 ohm---50 ohm line---+---291.4 ohm line---291.4 ohm SGCL1 --Prev1 | SGCL2 What is Pref1 before SGCL2 is turned on? What is Pref1 after SGCL2 is turned on? Did Pref1 change after SGCL2 is turned on? Since Pref1 *NEVER* encounters the impedance discontinuity how can it possibly be affected by SGCL2 being turned on? This is a perfect example of wave interaction. -- 73, Cecil http://www.w5dxp.com It's not an example of anything other than newsgroup rhetoric, Cecil. Buy a good RF data acquisition system, all the equipment listed in your problem, and run the experiment. I'd be happy to discuss the results with you afterward. 73, Jim AC6XG |
Analyzing Stub Matching with Reflection Coefficients
Jim Kelley wrote:
It's not an example of anything other than newsgroup rhetoric, Cecil. Buy a good RF data acquisition system, all the equipment listed in your problem, and run the experiment. I'd be happy to discuss the results with you afterward. Translation: I am clueless to explain one of the most simple of experiments involving s-parameters. -- 73, Cecil http://www.w5dxp.com |
Analyzing Stub Matching with Reflection Coefficients
Cecil Moore wrote:
Keith Dysart wrote: If the zero power point is stationary then no energy can be flowing. Time for you to review EM waves, Keith. There is a zero power point in every EM traveling wave every 1/2WL where the E-field and H-field are both zero at the same time. Cecil, Four questions: * Does your IEEE dictionary have an entry for "stationary"? * Which part of "every EM traveling wave" is stationary? * Do you actually read any of the messages to which you respond? * Do you want to retract your answer? 8-) 73, Gene W4SZ |
Analyzing Stub Matching with Reflection Coefficients
Cecil Moore wrote:
Gene Fuller wrote: You are going to pull a brain muscle by stretching so much. Are you suggesting that two wiggling points on a web page are the key to understanding the universe? No, just wave cancellation. If the graphic is completely incorrect, as you say, why did they publish it? Cecil, I did not say the graphic was incorrect, but rather that it is irrelevant. It correctly shows the addition of two sine waves. Big deal. 73, Gene W4SZ |
Analyzing Stub Matching with Reflection Coefficients
Gene Fuller wrote:
* Does your IEEE dictionary have an entry for "stationary"? I'm afraid you have been taken in by my devil's advocate argument based on Keith's faulty concepts. If what he says is true about standing waves, then the same concepts apply to traveling waves. If there are no traveling wave energy components being transferred when two traveling waves are flowing in opposite directions, then it logically follows that there can be no traveling wave energy component being transferred when one traveling wave is flowing in one direction. The *NET* energy flow is zero in a standing wave. But the component energy flow in the underlying EM waves is alive and well and flowing right through those current and voltage nodes without even knowing that they are there. The illusion of zero energy flow in EM traveling waves is one of the problems with shortcuts. EM waves have a set of boundary conditions that must be satisfied for them to exist. One of those conditions is that they must necessarily travel at c(VF). "Stationary" is not possible for any single EM wave. Nobody has been able to provide an example of a standing wave without the underlying forward and reverse EM traveling wave components (not even you) :-). Another condition for the existence of an EM traveling wave is that it has an associated energy level without which it cannot exist. A stationary EM wave is a contradiction in terms, an oxymoron. EM waves cannot stand still and exist only as a concept in the human mind. It is an illusionary temporarily superposed profile of two waves that, in reality, are moving in opposite directions at c(VF) and have absolutely *NO* effect on each other. The forward EM wave possesses direction and momentum that doesn't change until it encounters a physical impedance discontinuity. The reverse EM wave possesses direction and momentum that doesn't change until it encounters a physical impedance discontinuity. Anything else would violate the laws of physics. -- 73, Cecil, w5dxp.com -- 73, Cecil http://www.w5dxp.com |
Analyzing Stub Matching with Reflection Coefficients
Gene Fuller wrote:
I did not say the graphic was incorrect, but rather that it is irrelevant. It correctly shows the addition of two sine waves. OK, if it is irrelevant, why did they publish it? Why do they talk about "redistribution" of energy in other directions during a destructive interference event? Doesn't changing the direction and momentum of a wave qualify as "interaction"? And when those two sine waves are coherent, of equal amplitude, and opposite phase, they permanently *CANCEL* each other. Doesn't that satisfy the definition of "interacting"? I see you have been strangely silent on my example of s11(a1) originating and flowing away from the impedance discontinuity only to be canceled by s12(a2) when it flows through the impedance discontinuity and encounters the s11(a1) wave flowing away from the impedance discontinuity. How can the effect of one wave on the other not be interaction when both are flowing away from the impedance discontinuity and are *NEVER* incident upon any impedance discontinuity? -- 73, Cecil http://www.w5dxp.com |
Analyzing Stub Matching with Reflection Coefficients
On Apr 23, 4:56 am, Cecil Moore wrote:
A stationary EM wave is a contradiction in terms, an oxymoron. It sounds just like a standing EM wave. :-) Anything else would violate the laws of physics. The funny thing is, if you knew how to apply that constraint to all of your claims, you wouldn't find yourself playing newsgroup Whack-a-Mole day all day. 73, Jim AC6XG |
Analyzing Stub Matching with Reflection Coefficients
Jim Kelley wrote:
Cecil Moore wrote: A stationary EM wave is a contradiction in terms, an oxymoron. It sounds just like a standing EM wave. :-) EM waves cannot stand still. They must necessarily move at the speed of light, c(VF). The illusion of a stationary EM wave is actually two EM waves moving in opposite directions at the speed of light. Both waves include all of the boundary conditions necessary for EM waves to exist. Again, if you can present an example of an EM standing wave devoid of the forward and reverse traveling wave components, now would be a good time. Anything else would violate the laws of physics. The funny thing is, if you knew how to apply that constraint to all of your claims, you wouldn't find yourself playing newsgroup Whack-a-Mole day all day. I just love it when you wax technical, Jim. -- 73, Cecil, http://www.qsl.net/w5dxp |
Analyzing Stub Matching with Reflection Coefficients
Cecil Moore wrote:
Gene Fuller wrote: * Does your IEEE dictionary have an entry for "stationary"? I'm afraid you have been taken in by my devil's advocate argument based on Keith's faulty concepts. If what he says is true about standing waves, then the same concepts apply to traveling waves. If there are no traveling wave energy components being transferred when two traveling waves are flowing in opposite directions, then it logically follows that there can be no traveling wave energy component being transferred when one traveling wave is flowing in one direction. The *NET* energy flow is zero in a standing wave. But the component energy flow in the underlying EM waves is alive and well and flowing right through those current and voltage nodes without even knowing that they are there. The illusion of zero energy flow in EM traveling waves is one of the problems with shortcuts. EM waves have a set of boundary conditions that must be satisfied for them to exist. One of those conditions is that they must necessarily travel at c(VF). "Stationary" is not possible for any single EM wave. Nobody has been able to provide an example of a standing wave without the underlying forward and reverse EM traveling wave components (not even you) :-). Another condition for the existence of an EM traveling wave is that it has an associated energy level without which it cannot exist. A stationary EM wave is a contradiction in terms, an oxymoron. EM waves cannot stand still and exist only as a concept in the human mind. It is an illusionary temporarily superposed profile of two waves that, in reality, are moving in opposite directions at c(VF) and have absolutely *NO* effect on each other. The forward EM wave possesses direction and momentum that doesn't change until it encounters a physical impedance discontinuity. The reverse EM wave possesses direction and momentum that doesn't change until it encounters a physical impedance discontinuity. Anything else would violate the laws of physics. -- 73, Cecil, w5dxp.com Cecil, Nobody said the "wave" was stationary, only the point of zero energy is stationary. You have again demonstrated that you are not reading and understanding. The *NET* paragraph above is simply unmitigated nonsense. It appears that mistaken notion is one of the root causes of your continuing confusion. Until you get over this bogus idea of colliding energy flows there is no hope for further enlightenment. 73, Gene W4SZ |
Analyzing Stub Matching with Reflection Coefficients
Cecil Moore wrote:
Gene Fuller wrote: I did not say the graphic was incorrect, but rather that it is irrelevant. It correctly shows the addition of two sine waves. OK, if it is irrelevant, why did they publish it? Why do they talk about "redistribution" of energy in other directions during a destructive interference event? Doesn't changing the direction and momentum of a wave qualify as "interaction"? And when those two sine waves are coherent, of equal amplitude, and opposite phase, they permanently *CANCEL* each other. Doesn't that satisfy the definition of "interacting"? I see you have been strangely silent on my example of s11(a1) originating and flowing away from the impedance discontinuity only to be canceled by s12(a2) when it flows through the impedance discontinuity and encounters the s11(a1) wave flowing away from the impedance discontinuity. How can the effect of one wave on the other not be interaction when both are flowing away from the impedance discontinuity and are *NEVER* incident upon any impedance discontinuity? Cecil, I did respond to your example. I referred you to the message from K7ITM. The answer is contained in his quote. Since you seemed to have missed that one, here is the conclusion. The waves you are trying to create and then quickly cancel, in delta-t, simply never existed. Problem solved. 73, Gene W4SZ |
Analyzing Stub Matching with Reflection Coefficients
On Apr 23, 7:56 am, Cecil Moore wrote:
Gene Fuller wrote: * Does your IEEE dictionary have an entry for "stationary"? I'm afraid you have been taken in by my devil's advocate argument based on Keith's faulty concepts. If what he says is true about standing waves, then the same concepts apply to traveling waves. It becomes clear from your posts that you have a wave centric view of these behaviours. It is often valuable to have more than one way to view a situation. Let me offer you another. While I will describe this view only for transmission lines, its equivalent in free space would be the Maxwell equations, so, knowing your support for Maxwell, you should find it attractive. The voltages and currents on a transmission line can be described with a collection of differential equations. When these differential eqations are solved for a set of boundary conditions, the results describe the voltage and current on the line as a function of time and location along the line. Were one to set up an ideal line (for simplicity), terminated in its characteristic impedance, the functions that describe the voltage and current on the line can be derived. Plugging in the time and location one can determine the voltage at that place and instance. The curious investigator will be tempted to plot the voltage for a particular time as a function of location. The resulting plot will be nicely sinusoidal. Were one to plot the result for deltaT later, one finds a plot with exactly the same shape, but slightly shifted. A movie would show this nice sinusoid shifting its location at a constant velocity. And our intrepid investigator names this a travelling wave, a convenient moniker. Let us consider another line. This one is open circuited. Solving the diffential equations that describe the line for these new boundary conditions produces a different set of functions of time and location. Plotting the function of voltage with respect to location again produces a sinusoid, but the amplitude depends on the selected time. This plot, when played as a movie, shows no sign of moving and our intrepid investigator names it a standing wave, another convenient moniker. But just because they are both called waves does not make them the same. One always has the same shape and amplitude and appears to move. The other shares the shape, does not move and has an amplitude that varies. Fundamentally, they are both just convenient visualizations of solutions from the same set of differential equations with different boundary conditions. For the standing wave, further arithmetic reveals that the function that expresses the voltage as a function of time and location can be simplified and made more useful if it is expressed in terms of two travelling waves, one from the left and one from the right. But this is just an alternate expression of the function that resulted from the solution of a set of differential equations. While the initial differential equations express voltage and current, one could certainly derive equations that expressed power, or energy storage, or whatever happened to be of interest. One could then solve these and the expression that results would be a function of time and location. Were one to solve the differential equation for power on the open circuited line at a location of a voltage null, the answer would be zero. And all computed without the need for forward and backward waves. --- So which is the truth? The differential equations or the forward and backward waves? Which analysis technique is more complete? And which is the alternative view that makes the problems solvable in reasonable time? It is clear to me that the differential equations rule, much as Maxwell's equations are considered the root for electric and magnetic fields. Travelling and standing waves are mere visualizations, though that visualization simplifies solving many problems. But forward and reverse waves are definitely not the foundation on which all else rests. ....Keith |
Analyzing Stub Matching with Reflection Coefficients
On Apr 23, 8:54 am, Gene Fuller wrote:
Cecil Moore wrote: Gene Fuller wrote: * Does your IEEE dictionary have an entry for "stationary"? I'm afraid you have been taken in by my devil's advocate argument based on Keith's faulty concepts. If what he says is true about standing waves, then the same concepts apply to traveling waves. If there are no traveling wave energy components being transferred when two traveling waves are flowing in opposite directions, then it logically follows that there can be no traveling wave energy component being transferred when one traveling wave is flowing in one direction. The *NET* energy flow is zero in a standing wave. But the component energy flow in the underlying EM waves is alive and well and flowing right through those current and voltage nodes without even knowing that they are there. The illusion of zero energy flow in EM traveling waves is one of the problems with shortcuts. EM waves have a set of boundary conditions that must be satisfied for them to exist. One of those conditions is that they must necessarily travel at c(VF). "Stationary" is not possible for any single EM wave. Nobody has been able to provide an example of a standing wave without the underlying forward and reverse EM traveling wave components (not even you) :-). Another condition for the existence of an EM traveling wave is that it has an associated energy level without which it cannot exist. A stationary EM wave is a contradiction in terms, an oxymoron. EM waves cannot stand still and exist only as a concept in the human mind. It is an illusionary temporarily superposed profile of two waves that, in reality, are moving in opposite directions at c(VF) and have absolutely *NO* effect on each other. The forward EM wave possesses direction and momentum that doesn't change until it encounters a physical impedance discontinuity. The reverse EM wave possesses direction and momentum that doesn't change until it encounters a physical impedance discontinuity. Anything else would violate the laws of physics. -- 73, Cecil, w5dxp.com Cecil, Nobody said the "wave" was stationary, only the point of zero energy is stationary. You have again demonstrated that you are not reading and understanding. I think he may be too busy having that strange kind of dream he talked about when he implicitly threw out at least 90% of all S-parameter analysis by saying that "reality requires complete reflection of the return wave at the interface between the [matched] source and the line." Either you believe in the superposition principle in linear systems, or you don't. He obviously doesn't. From the lab, Bunsen |
Analyzing Stub Matching with Reflection Coefficients
Gene Fuller wrote:
The *NET* paragraph above is simply unmitigated nonsense. It appears that mistaken notion is one of the root causes of your continuing confusion. Until you get over this bogus idea of colliding energy flows there is no hope for further enlightenment. If colliding energy doesn't flow, then waves interact away from an impedance discontinuity since the colliding energy components are in separate EM waves traveling in opposite directions. Which will it be? You cannot have it both ways. 1. The ExB joules/sec components in the forward wave and the reflected wave pass through each other with no interaction such that the *NET* energy flow is zero. 2. The ExB joules/sec components flowing in each direction cause all energy to stop flowing because of wave interaction. Please tell us which one is true and which one is false. -- 73, Cecil, http://www.qsl.net/w5dxp |
Analyzing Stub Matching with Reflection Coefficients
Gene Fuller wrote:
The waves you are trying to create and then quickly cancel, in delta-t, simply never existed. Problem solved. Problem solved by rendering an s-parameter analysis invalid? b1 = s11(a1) + s12(a2) = 0 So s11(a1) and s12(a2) in the s-parameter equations don't exist and never existed. Don't you think you should tell HP so they can change their Ap Notes? -- 73, Cecil, http://www.qsl.net/w5dxp |
Analyzing Stub Matching with Reflection Coefficients
Keith Dysart wrote:
Were one to solve the differential equation for power on the open circuited line at a location of a voltage null, the answer would be zero. And all computed without the need for forward and backward waves. The *NET* power at any point on a lossless stub is zero so that is no big deal. The standing wave current is always 90 degrees out of phase with the standing wave current so cos(90) = 0. At a voltage node, all of the energy has simply moved into the magnetic field. Calculate the number of electromagnetic joules in the line and get back to us on how they are reflected from your above purely virtual impedance at a voltage "null" and how they can even exist without a velocity of c(VF). -- 73, Cecil, http://www.qsl.net/w5dxp |
Analyzing Stub Matching with Reflection Coefficients
Dr. Honeydew wrote:
Either you believe in the superposition principle in linear systems, or you don't. He obviously doesn't. Superposition is known to fail in nonlinear systems. A source is obviously not linear. The V/I of an active dynamic source resists any attempt at linear superposition. How does your superposition work when you try to spit up a fire hose? -- 73, Cecil, http://www.qsl.net/w5dxp |
Analyzing Stub Matching with Reflection Coefficients
Cecil Moore wrote:
The *NET* power at any point on a lossless stub is zero so that is no big deal. The standing wave current is always 90 degrees out of phase with the standing wave current so cos(90) = 0. At a voltage node, all of the energy has simply moved into the magnetic field. With 4 amps of RF current at that voltage "null", how could zero joules/sec possibly exist at that point? Methinks there are some I^2*Z0 joules/sec in that 4 amps of RF EM current that necessarily must be traveling at c(VF). -- 73, Cecil, http://www.qsl.net/w5dxp |
Analyzing Stub Matching with Reflection Coefficients
Cecil Moore wrote:
Dr. Honeydew wrote: Either you believe in the superposition principle in linear systems, or you don't. He obviously doesn't. Superposition is known to fail in nonlinear systems. A source is obviously not linear. Sources are linear. Consider the classic voltage source.. it has zero impedance. You can stack as many voltage sources as you like, and the voltage at the top of the stack is the same as the sum of the individual voltages. The V/I of an active dynamic source resists any attempt at linear superposition. - a practical RF source, perhaps, might be nonlinear, although it's pretty easy to come close.. Consider an oscillator isolated by an isolator or a big pad. How does your superposition work when you try to spit up a fire hose? Just fine. No different than receiving a faint signal superimposed on a large interfering signal at a different frequency. |
Analyzing Stub Matching with Reflection Coefficients
Cecil Moore wrote:
Jim Kelley wrote: Cecil Moore wrote: A stationary EM wave is a contradiction in terms, an oxymoron. It sounds just like a standing EM wave. :-) Again, if you can present an example of an EM standing wave devoid of the forward and reverse traveling wave components, now would be a good time. I didn't say anything was devoid of anything, Cecil. I just said your description of a stationary EM wave sounds just like a standing EM wave. I don't think you caught my drift (or Gene's), but go ahead and give it another whack. 73, Jim AC6XG |
Analyzing Stub Matching with Reflection Coefficients
Cecil Moore wrote:
Gene Fuller wrote: The waves you are trying to create and then quickly cancel, in delta-t, simply never existed. Problem solved. Problem solved by rendering an s-parameter analysis invalid? b1 = s11(a1) + s12(a2) = 0 So s11(a1) and s12(a2) in the s-parameter equations don't exist and never existed. Don't you think you should tell HP so they can change their Ap Notes? Cecil, You routinely confuse results and observations with underlying causes. There is nothing wrong with s-parameter analysis. The problem is that you keep trying to make s-parameters something they are not. Did you perhaps notice that word "parameter"? Do you think there might be a reason that term was chosen rather than, say, "all encompassing equations describing the entire universe"? S-parameters work fine for their intended purpose. However, they don't trump Maxwell's equations or solid state physics, nor do they try to. 73, Gene W4SZ |
Analyzing Stub Matching with Reflection Coefficients
Cecil Moore wrote:
Gene Fuller wrote: The *NET* paragraph above is simply unmitigated nonsense. It appears that mistaken notion is one of the root causes of your continuing confusion. Until you get over this bogus idea of colliding energy flows there is no hope for further enlightenment. If colliding energy doesn't flow, then waves interact away from an impedance discontinuity since the colliding energy components are in separate EM waves traveling in opposite directions. Which will it be? You cannot have it both ways. 1. The ExB joules/sec components in the forward wave and the reflected wave pass through each other with no interaction such that the *NET* energy flow is zero. 2. The ExB joules/sec components flowing in each direction cause all energy to stop flowing because of wave interaction. Please tell us which one is true and which one is false. Cecil, You still don't believe in superposition, do you? I don't need to worry about which of your purported answers is goofier than the other. Superposition allows me to combine your traveling waves into a standing wave. The energy analysis then becomes very easy, with no paradoxes. 73, Gene W4SZ |
Analyzing Stub Matching with Reflection Coefficients
Cecil Moore wrote: Gene Fuller wrote: The waves you are trying to create and then quickly cancel, in delta-t, simply never existed. Problem solved. Problem solved by rendering an s-parameter analysis invalid? b1 = s11(a1) + s12(a2) = 0 So s11(a1) and s12(a2) in the s-parameter equations don't exist and never existed. Don't you think you should tell HP so they can change their Ap Notes? HP would simply observe that what b1 = 0 means is that there is no energy and there are no waves moving in the direction of b1. 73, Jim AC6XG |
Analyzing Stub Matching with Reflection Coefficients
Jim Lux wrote:
Sources are linear. Consider the classic voltage source. it has zero impedance. You talk about those sources as if they exist in reality. They only exist in a human mind in a mathematical model. a practical RF source, perhaps, might be nonlinear, although it's pretty easy to come close.. Consider an oscillator isolated by an isolator or a big pad. I have suggested those configurations myself and those ideas have been rejected by the other side - which claims that all one needs to linearize a real-world source is a ten cent resistor. How does your superposition work when you try to spit up a fire hose? Just fine. No different than receiving a faint signal superimposed on a large interfering signal at a different frequency. Do you really think that any of those spit molecules make it all the way to the source? -- 73, Cecil, http://www.qsl.net/w5dxp |
Analyzing Stub Matching with Reflection Coefficients
Gene Fuller wrote:
There is nothing wrong with s-parameter analysis. There is certainly something wrong with it if the terms in the s-parameter never existed, as you assert. S-parameters work fine for their intended purpose. However, they don't trump Maxwell's equations or solid state physics, nor do they try to. Nobody said they did, Gene, so this is just another one of your straw men. EM waves canceling each other to zero are perfectly compatible with Maxwell's equations. When you use Maxwell's equations on two EM waves of equal amplitude and opposite phase, do those equations really say that the two waves, as you assert, never existed in the first place? -- 73, Cecil, http://www.qsl.net/w5dxp |
Analyzing Stub Matching with Reflection Coefficients
Gene Fuller wrote:
I don't need to worry about which of your purported answers is goofier than the other. Superposition allows me to combine your traveling waves into a standing wave. The energy analysis then becomes very easy, with no paradoxes. You yourself have said that nothing is lost during superposition. Presumably that includes energy not being destroyed. Given that |s11(a1)|^2 = 1 joule/sec Given that |s12(a2)|^2 = 1 joule/sec Given that |b1|^2 = 0 What happened to the 2 joules/sec? -- 73, Cecil, http://www.qsl.net/w5dxp |
Analyzing Stub Matching with Reflection Coefficients
Jim Kelley wrote:
HP would simply observe that what b1 = 0 means is that there is no energy and there are no waves moving in the direction of b1. Yes, and HF also observes that, e.g.: |s11(a1)|^2 = 1 joule/sec |s12(a2)|^2 = 1 joule/sec Presumably, HP doesn't believe in destruction of energy. Hecht says those joules existed with a direction and momentum toward the source. What happened to those joules to reverse their direction and momentum? -- 73, Cecil, http://www.qsl.net/w5dxp |
Analyzing Stub Matching with Reflection Coefficients
Cecil Moore wrote: Jim Kelley wrote: HP would simply observe that what b1 = 0 means is that there is no energy and there are no waves moving in the direction of b1. Yes, and HF also observes that, e.g.: |s11(a1)|^2 = 1 joule/sec |s12(a2)|^2 = 1 joule/sec I don't think they do. Presumably, HP doesn't believe in destruction of energy. I'm quite sure that's true, which is why they wouldn't agree with your "e.g." above. Hecht says those joules existed with a direction and momentum toward the source. Actually, he never does say that. What happened to those joules to reverse their direction and momentum? Clearly, according to everything that is known and is measurable, those joules are not traveling in the direction you claim. 73, Jim AC6XG |
Analyzing Stub Matching with Reflection Coefficients
On Apr 23, 10:23 am, Cecil Moore wrote:
Dr. Honeydew wrote: Either you believe in the superposition principle in linear systems, or you don't. He obviously doesn't. Superposition is known to fail in nonlinear systems. A source is obviously not linear. The V/I of an active dynamic source resists any attempt at linear superposition. So you don't believe in any of the S-parameter analysis done on linear small-signal amplifiers, then. Might as well just toss HP AN95 in the trash. Might as well toss the S parameters provided by pretty much all the RF transistor manufacturers in the trash. And in fact, even beyond that, you don't believe in any of the S-paramter analysis done on any system that's propagating power, because that power came from a source, and if you toss one non-linear element into the system, the whole system is non-linear and none of this linear systems analysis would be valid. Enjoy your dreams, whatever kind they may be. Fortunately, they won't keep the rest of us from continuing to successfully analyze our systems, including the sources, with H parameters, Y parameters, S parameters, or just plain old elemental linear circuit theory. From the labs, Bunsen |
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