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On Tue, 1 Jan 2008 18:44:17 -0800 (PST), Keith Dysart
wrote: Since the experiment ends before the reflection returns to the generator, Is it a step, or is it a pulse? Makes a huge difference in the analysis. the impedance of the generator is irrelevant. The impedance perhaps, but not the voltage. I specifically offered a difference of sources (Norton vs. Thevenin). The impedance is the same either way, the voltage is not. As you introduce power later in this response, power at the source is even more contentious. As such, we can drop this altogether. Ah. The challenge of written precisely. Consider the generator to be on the left end of the line and the open to be at the right end. When the capacitance at the right end charges to 2 * V, the current now has to stop a little bit more to the left. Still doesn't make sense, and I wouldn't attribute it to precision seeing that you've written the same thing twice. Again, the poor writing meant a bit further to left from the end. Yes, if you are in a left-right progression, further is more to the right. There is the ambiguity of "end effect." Want to explain how you double the stored voltage in the distributed capacitance of the line without current? * The energy formerly present in the inductance of the line has been transferred to the capacitance. That is always so. You haven't offered anything differentiable from always, where previously (and later in your response, here) you suggested current stopped flowing even when voltage was doubling. The definition of capacitance is explicitly found in the number of electrons (charge or energy) on a surface; which in this case has not changed.The charge that is continuing to flow from the source is being used to charge the distributed capacitance of the line. It would appear now that charge is flowing again, but that there is a confusion as to where the flow comes from. * Using the new reference scheme, What new reference scheme? charge to the left of the leftward propagating step continues to flow, while charge to the right has stopped flowing. If precision was ever called for, now is the time. Why would the source at less voltage provide current to flow into a cap that is rising in potential above it? * The beauty of inductance. You get extra voltage when you try to stop the flow. You don't explain where the extra voltage is. There is a double voltage to be sure, but you have not exactly drawn a cause-and-effect relationship. Challenges with the referent. The former view is that a voltage of 2*V is propagating back along the line. The latter view is that it is a step of V above the already present V. Sounds more like a problem for the challenged (i.e. there is no difference between 2*V and V+V). In this model, the step function has propagated to the end, been reflected and is now propagating backwards. Implicit in this description is that the step continues to flow to the end of the line and be reflected as the leading edge travels back to the source. This is a difficult read. *You have two sentences. *Is the second merely restating what was in the first, or describing a new condition (the reflection)? Agreed. What is a good word to describe the constant voltage that follows the actual step change in voltage? The "tread" perhaps? Does it matter? It is another step. That should be obvious for the sake of superposition. "The tread continues to flow to the end of the line and be reflected as the leading edge travels back to the source." I am not sure that that is any clearer. Not particularly, since we now have three things moving: 1. Step; 2. Tread; 3. Leading Edge. It would seem to me that both 1 and 2 have a 3; so what are you trying to say with the novel introduction of two more terms? And this is the major weakness in the model. Which model? * The "no interaction" model. And which model is the "no interaction" model? The former, or the latter? The latter? or the former? It claims the step function is still flowing in the portion of the line that has a voltage of 2*V and *zero* current. Does a step function flow? * Perhaps the "tread"? But then should the step change be called the "riser"? So now we have four things moving: 1. Step; 2. Tread; 3. Leading Edge. 4. Riser It would seem to me that both 1,2 and 4 have a 3; so what are you trying to say with the novel introduction of three more terms? As for "zero" current, that never made sense in context here. Somewhat clarified, I hope. But for clarity, the current to the right of the leftward propagating step is zero. So now the leftward propagating step is 1. Step; 2. Tread; 3. Leading Edge; 4. Riser? If I simply discard the last three invented terms; went out on the thin limb of interpretation; then, in my mind's eye I would see that, yes, no current is flowing to the physical right of the transient (the only thing that is moving - as evidenced through voltage). A trivial example is connecting to 10 volt batteries in parallel through *a .001 ohm resistor. Parallel has two outcomes, which one? *"Through" a resistor to WHERE? In series? *In parallel? * Much to ambiguous. I know. Trying to conserve words leads to confusion. Try: negative to negative, positives connected using the resistor. Makes quite a difference. Perhaps not in the math, but certainly in the concept. However, by this forced march through the math, it appears there are two batteries in parallel; (series) bucking; with a parallel resistor. So in the end, successful communication of the schematic. Actually no. You describe a resistor in a series loop; I describe a resistor in parallel. Consider the repetition of your last statement above: positives connected using the resistor. Positives connected through the resistor (the sense of "using" the resistor as connector)? Or positives connected, then using the resistor (where it is also connected, but unstated as such) to the negatives? It would seem if you knew the charge, you already know the energy; but the power? Just energy per unit time. We know the energy distribution on the line, so we know the power at any point and time. Time has not been quantified, whereas voltage, hence charge, hence energy has. Why introduce a new topic without enumerating it, when its inclusion adds nothing anyway? You don't develop anything that explains the step in terms of power. You don't use power anywhere. In fact we then step into the philosophy of does a line actually move power, or energy? That debate would cloud any issue of a step's migration, reflection, or any of a spectrum of characteristics that power has no sway over. But when two waves are simultaneously present, it is only legal to superpose the voltage and the current. And illegal if only one is present? * No. Legal to also compute the power. Please note you start your sentence with a "But." Sentences (much less paragraphs) are not started with coordinating conjunctions. When you use "but," the logical implication is that you are coordinating: two-waves with an equal ranking and unexpressed: one-wave. One may also use "but" at the beginning of a sentence as a logical connector between equal ideas (a transitional adverb); however, you don't have anything in the preceding, original paragraph other than a single wave. I do not see anything distinctive about two waves over one wave until your recent injection of power (not at all in the original), and to no effect except to raise the objection (rather circular and unnecessary inclusions to abandon the discussion of reflection in rhetorical limbo). Apparently your transition spans many postings to a festering point by Cecil (this is, of course, another one of my interpretations). Earlier you asked for an experiment. How about this one.... Take two step function generators, one at each end of a transmission line. Start a step from each end at the same time. When the steps collide in the middle, the steps can be viewed as passing each other without interaction, or reversing and propagating back to their respective sources. Why just that particular view? Those seem to be the common alternatives. If there are more, please share. Neither view works. We can measure the current at the middle of the line and observe that it is always 0. Is it? *When? Always. You seem to be in self-contradiction when you describe voltage doubles without current flow. If, for some infinitesimal line section, there is no current through it, then there is no potential difference across it. Or did you mean along it? A point well made in the scheme of precise language. Yet and all, taken singly (one/either conductor) or doubly (a transmission line section); then the identical statement remains true with both interpretations for the step condition. Of course, a lot may be riding on whether you are speaking of a step function, or a pulse. Seeing the original was explicit to step, and never introduces pulse; then there is no current flow as I responded: Hence, the when is some infinitesimal time before the waves of equal potential meet - and no current flow forever after. Therefore the charge that is filling the capacitance and causing the voltage step which is propagating back towards each generator How did that happen? *No potential difference across an infinitesimal line section, both sides at full potential (capacitors fully charged, or charging at identical rates). *Potentials on either side of the infinitesimal line section are equal to each other and to the sources, hence no potential differences anywhere, *No potential differences, no current flow, no charge change, no reflection, no more wave. The last bit of induction went to filling the last capacitance element with the last charge of current. *Last gasp. *No more gas. *Nothing left. Finis. must be coming from the generator to which the step is propagatig because no charge is crossing the middle of the line. Do you like it? Not particularly. *What does it demonstrate? That they bounce rather than pass silently. How do you introduce recoil or maintain momentum without energy? Odd. Please remove my need to perform interpretation and give me a more succinct accounting. Further, limit this to one scenario (this last failed example is certainly dead in the water as far as collisions go). 73's Richard Clark, KB7QHC |
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