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![]() "Dave" wrote in message news:q7u8j.6941$xd.2942@trndny03... "Roger" wrote in message . .. Richard Clark wrote: On Thu, 13 Dec 2007 08:40:53 -0800, Roger wrote: And just for completeness... The fundamental equations also work when: - the signal is not sinusoidal, e.g. pulse, step, square, ... - rather than a load at one end, there is a source at each end - the sources at each end produce different arbitrary functions - the arbitrary functions at each end are DC sources It is highly instructive to compute the forward and reverse voltage and current (and then power) for a line with the same DC voltage applied to each end. ...Keith ...Keith Interesting! The important thing is to get answers that agree with our experiments. I have done some computations for DC voltage applied to transmission lines. The real surprise for me came when I realized that transmission line impedance could be expressed as a function of capacitance and the wave velocity. Z0 = 1/cC where c is the velocity of the wave and C is the capacitance of the transmission line per unit length. Hi Roger, This last round has piqued my interest when we dipped into DC. Those "formulas" would lead us to a DC wave velocity? 73's Richard Clark, KB7QHC Hi Richard, Here are two links to pages that cover the derivation of the formula Zo = 1/cC and much more. http://www.speedingedge.com/PDF-File..._Impedance.pdf http://www.ece.uci.edu/docs/hspice/h...001_2-269.html Here is the way I proposed to Kevin Schmidt nearly seven years ago after seeing him use the formula on a web page: *ASSUME*: 1) An electrical wave travels at the speed of light, c 2) A 'perfect' voltage source without impedance, V 3) A 'perfect' transmission line having no resistance but uniform capacitance per unit length, C *CONDITIONS AND SOLUTION* The perfect voltage source has one terminal connected to the transmission line prior to beginning the experiment. The experiment begins by connecting the second terminal to the transmission line. The voltage source drives an electrical wave down the transmission line at the speed of light. Because of the limitation of speed, the wave travels in the shape of a square wave containing all frequencies required to create a square wave. The square wave travels down the transmission line at the speed of light (c). After time (T), the wave has traveled distance cT down the transmission line, and has charged the distributed capacity CcT of the line to voltage V over that distance. The total charge Q on the distributed capacitor is VCcT. Current (I) is expressed as charge Q per unit time. Therefore the current into the transmission line can be expressed as I = Q/T = VCcT / T = VCc Impedance (Zo) is the ratio of voltage (V) to current (I). Therefore the impedance can be expressed as Zo = V / I = V / VCc = 1/Cc We can generalize this by using the velocity of the electrical wave rather than the speed of light, which allows the formula to be applied to transmission line with velocities slower than the speed of light. Of course, only the wave front and wave end of a DC wave can be measured to have a velocity. 73, Roger, W7WKB the OBVIOUS error is that the step when the second terminal is connected DOES NOT travel down the line at c, it travels at some smaller percentage of c given by the velocity factor of the line. That IS what I said. Think of the velocity as a moving wall, with the capacitor charged behind the wall, uncharged in front of the moving wall. The second OBVIOUS error is the terminology 'DC wave'. you are measuring the propagation velocity of a step function. this is a well defined fields and waves 101 homework problem, not to be confused with the much more common 'sinusoidal stead state' solution that most other arguments on this group assume but don't understand. Be real. This experiment can be performed, and the DC switched as frequently as desired. How square the wave front will be depends upon real world factors. Go to a transmission line characteristics table and use the formula to compare Zo, capacity per length, and line velocity. It will amaze you. 73, Roger, W7WKB |
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On Fri, 14 Dec 2007 05:18:03 -0800, "Roger Sparks"
wrote: That IS what I said. Think of the velocity as a moving wall, with the capacitor charged behind the wall, uncharged in front of the moving wall. .... Be real. This experiment can be performed, and the DC switched as frequently as desired. How square the wave front will be depends upon real world factors. Go to a transmission line characteristics table and use the formula to compare Zo, capacity per length, and line velocity. It will amaze you. Hi Roger, Take a deep breath, exhale, give what's above some more thought in light of many objections. Now, tells us just what significance any of this has in relation to already well established line mechanics? It certainly isn't different within the confines of its limitations if that is what you are trying to impress upon the group. I suppose for a mental short-cut it has some appeal, we get too many theories here based on approximations to stricter math. One such example is when an equation of approximation has forgotten the underlying |absolute value| and suddenly an inventor arrives with a "new" theory that discovers uses for negative solutions. Further, there is nothing DC about it at all. DC is either static (and in spite of Arthur's corruption of the term, that means no movement whatever) or it is a constant unvarying current. A succession of distributed capacitors rules unvarying current out (and if it isn't already obvious, those unmentioned distributed inductors in one of your links do too) - hence the step, hence the infinity of waves, and from this, real world dispersion which kills the step enough to make that varying current apparent enough so as to remove all doubt. 73's Richard Clark, KB7QHC |
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Richard Clark wrote:
On Fri, 14 Dec 2007 05:18:03 -0800, "Roger Sparks" wrote: That IS what I said. Think of the velocity as a moving wall, with the capacitor charged behind the wall, uncharged in front of the moving wall. .... Be real. This experiment can be performed, and the DC switched as frequently as desired. How square the wave front will be depends upon real world factors. Go to a transmission line characteristics table and use the formula to compare Zo, capacity per length, and line velocity. It will amaze you. Hi Roger, Take a deep breath, exhale, give what's above some more thought in light of many objections. Now, tells us just what significance any of this has in relation to already well established line mechanics? It certainly isn't different within the confines of its limitations if that is what you are trying to impress upon the group. I suppose for a mental short-cut it has some appeal, we get too many theories here based on approximations to stricter math. One such example is when an equation of approximation has forgotten the underlying |absolute value| and suddenly an inventor arrives with a "new" theory that discovers uses for negative solutions. Further, there is nothing DC about it at all. DC is either static (and in spite of Arthur's corruption of the term, that means no movement whatever) or it is a constant unvarying current. A succession of distributed capacitors rules unvarying current out (and if it isn't already obvious, those unmentioned distributed inductors in one of your links do too) - hence the step, hence the infinity of waves, and from this, real world dispersion which kills the step enough to make that varying current apparent enough so as to remove all doubt. 73's Richard Clark, KB7QHC Hi Richard, The math seems to work, but if you have no use for it, disregard it. On the other hand, if another perspective of electro magnetics that conforms to traditional mathematics can provide additional insight, use it. I am surprised at your criticism in using DC. To me, a square wave is DC for a short time period. Is the observation that a square wave can be described as a series of sine waves troubling to you? Perhaps the observation that a square wave might include waves of a frequency so high that they would not be confined in a normal transmission line is surprising or troubling to you? My goal is to better understand electromagnetic phenomena. You have given some very astute insight many times in the past and thanks for that. Negative comment is equally valuable, but sometimes a little harder to swallow. 73, Roger, W7WKB |
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On Fri, 14 Dec 2007 09:45:04 -0800, Roger wrote:
Hi Richard, The math seems to work, but if you have no use for it, disregard it. On the other hand, if another perspective of electro magnetics that conforms to traditional mathematics can provide additional insight, use it. Hi Roger, This does not answer why TWO mathematics (both traditional) are needed, especially since one is clearly an approximation of the other, and yet offers no obvious advantage. I've already spoken to the hazards of approximations being elevated to proof by well-meaning, but slightly talented amateurs. I am surprised at your criticism in using DC. To me, a square wave is DC for a short time period. This single statement, alone, is enough to be self-negating. You could as easily call a car with a standard stick shift an automatic between the times you use the clutch - but that won't sell cars, will it? Is the observation that a square wave can be described as a series of sine waves troubling to you? Perhaps the observation that a square wave might include waves of a frequency so high that they would not be confined in a normal transmission line is surprising or troubling to you? DC as sine waves is not a contradiction on the face of it? DC that consists of waves of a frequency so high that it would not be confined in a normal transmission line is very surprising, isn't it? Would it surprise you to find your batteries in their packaging direct from the store are radiating on the shelf? They are DC, are they not? If the arguments of your sources works for an infinite line, they must be equally true for an infinitesimal open line. When your headlights are on, do they set off radar detectors in cars nearby because of the high frequencies now associated with DC? My goal is to better understand electromagnetic phenomena. You have given some very astute insight many times in the past and thanks for that. Negative comment is equally valuable, but sometimes a little harder to swallow. The pollution of terms such as DC to serve a metaphor that replaces conventional line mechanics is too shallow glass to attempt to quench any thirst. The puzzle here is the insistence on hugging DC, when every element of all of your links could as easily substitute Stepped Wave and remove objections. The snake in the wood pile is once having fudged what DC means, it is only a sideways argument away from rendering the term DC useless. Is the term Stepped Wave (the convention) anathema for a leveraging the novel origination (the invention) of DC Wave? 73's Richard Clark, KB7QHC |
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Richard Clark wrote:
The puzzle here is the insistence on hugging DC, when every element of all of your links could as easily substitute Stepped Wave and remove objections. How about "continuous wave" for Morse code? -- 73, Cecil http://www.w5dxp.com |
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Richard Clark wrote:
On Fri, 14 Dec 2007 09:45:04 -0800, Roger wrote: Hi Richard, The math seems to work, but if you have no use for it, disregard it. On the other hand, if another perspective of electro magnetics that conforms to traditional mathematics can provide additional insight, use it. Hi Roger, This does not answer why TWO mathematics (both traditional) are needed, especially since one is clearly an approximation of the other, and yet offers no obvious advantage. I've already spoken to the hazards of approximations being elevated to proof by well-meaning, but slightly talented amateurs. The derivation did several things for me. It clearly explains why we do not have a runaway current when we first connect a voltage to a transmission line, what transmission line impedance is, that moving particles can not be the entire explanation for the electromagnetic wave (because the energy field moves much faster than the electrons), and puts into place a richer understanding of inductance. I am surprised at your criticism in using DC. To me, a square wave is DC for a short time period. This single statement, alone, is enough to be self-negating. You could as easily call a car with a standard stick shift an automatic between the times you use the clutch - but that won't sell cars, will it? We could use the concept of a stepped wave, but that would imply the need for several steps to develop the formula. Only the square wave front and continued charge maintenance is required, observations that can be easily verified by experiment. Is the observation that a square wave can be described as a series of sine waves troubling to you? Perhaps the observation that a square wave might include waves of a frequency so high that they would not be confined in a normal transmission line is surprising or troubling to you? DC as sine waves is not a contradiction on the face of it? DC that consists of waves of a frequency so high that it would not be confined in a normal transmission line is very surprising, isn't it? What is your point here? Are implying that the formula is incorrect because a sine wave was not mentioned in the derivation. I am sure that all of the sophisticated readers of this news group understand that the sharp corner of the square wave is composed of ever higher frequency waves. This leads Cecil to comment that the leading edge of a square wave could be composed of photons, which is a valid observation. It also explains your observation that true square waves are not possible (I am paraphrasing your comments) because of dispersion. It is interesting to run an FFT on a square wave to see how the frequencies can be resolved. Would it surprise you to find your batteries in their packaging direct from the store are radiating on the shelf? They are DC, are they not? If the arguments of your sources works for an infinite line, they must be equally true for an infinitesimal open line. When your headlights are on, do they set off radar detectors in cars nearby because of the high frequencies now associated with DC? They only set off the radar detectors when I turn them on and off. I have high power lights!! A lightning strike is a much better example of DC containing high frequencies. My goal is to better understand electromagnetic phenomena. You have given some very astute insight many times in the past and thanks for that. Negative comment is equally valuable, but sometimes a little harder to swallow. The pollution of terms such as DC to serve a metaphor that replaces conventional line mechanics is too shallow glass to attempt to quench any thirst. The puzzle here is the insistence on hugging DC, when every element of all of your links could as easily substitute Stepped Wave and remove objections. The snake in the wood pile is once having fudged what DC means, it is only a sideways argument away from rendering the term DC useless. Is the term Stepped Wave (the convention) anathema for a leveraging the novel origination (the invention) of DC Wave? 73's Richard Clark, KB7QHC We would complicate the concept and thereby begin to confuse people if we insisted on using the "Stepped Wave" term. It is a simple step to recognize that if we can make a wave front with one battery, we can use a lot of batteries and carefully place and switch them to form a sine wave. The more batteries and switches, the better the representation. Is there some harm in considering Zo = 1/cC? It should only add to the tools we have to explain electromagnetic waves. 73, Roger, W7WKB |
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![]() Is there some harm in considering Zo = 1/cC? It should only add to the tools we have to explain electromagnetic waves. 73, Roger, W7WKB yes. because its WRONG. you have made an assumption that is not realistic for any transmission line. There is no way a transmission line can have a velocity factor of 1.0, just can't happen... all the equations fall apart and become meaningless at that point. there is a reason for the velocity factor, or beta, depending on which you prefer. learn it, and use it properly, and it will serve you well. |
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On Fri, 14 Dec 2007 11:35:25 -0800, Roger wrote:
The derivation did several things for me. It clearly explains why we do not have a runaway current when we first connect a voltage to a transmission line, Hi Roger, It doesn't describe why the current flows in the first place, does it? what transmission line impedance is, that moving particles can not be the entire explanation for the electromagnetic wave (because the energy field moves much faster than the electrons), and puts into place a richer understanding of inductance. And here we begin on the wonderful world of spiraling explanations, not found in the original source: "Moving particles cannot be the entire explanation?" How about that in the first place, particles don't inhabit the explanation at all? What is your point here? Are implying that the formula is incorrect because a sine wave was not mentioned in the derivation. I am sure that all of the sophisticated readers of this news group understand that the sharp corner of the square wave is composed of ever higher frequency waves. I'm even convinced most of them would not call this DC too. We would complicate the concept and thereby begin to confuse people if we insisted on using the "Stepped Wave" term. They would've been confused anyway. It is a simple step to recognize that if we can make a wave front with one battery, we can use a lot of batteries and carefully place and switch them to form a sine wave. The more batteries and switches, the better the representation. And this is still DC? Is there some harm in considering Zo = 1/cC? This is best left in the privacy of the home. However, none of your comments respond to the question: What is with this death grip on DC? What makes it so important that it be so tightly wedded to Waves? What mystery of the cosmos is answered with this union that has so long escaped the notice of centuries of trained thought? 73's Richard Clark, KB7QHC |
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Richard Clark wrote:
How about that in the first place, particles don't inhabit the explanation at all? How about quantum physics telling us that nothing except particles exist? You really want to take on the body of quantum physics and physicists? -- 73, Cecil http://www.w5dxp.com |
#10
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Richard Clark wrote:
On Fri, 14 Dec 2007 11:35:25 -0800, Roger wrote: The derivation did several things for me. It clearly explains why we do not have a runaway current when we first connect a voltage to a transmission line, Hi Roger, It doesn't describe why the current flows in the first place, does it? Are you asking for a discussion about batteries? what transmission line impedance is, that moving particles can not be the entire explanation for the electromagnetic wave (because the energy field moves much faster than the electrons), and puts into place a richer understanding of inductance. And here we begin on the wonderful world of spiraling explanations, not found in the original source: "Moving particles cannot be the entire explanation?" How about that in the first place, particles don't inhabit the explanation at all? You originally asked what I learned from Zo = 1/cC. What I learn from it may not be obvious to you. Discussing particles would be a completely new discussion. What is your point here? Are implying that the formula is incorrect because a sine wave was not mentioned in the derivation. I am sure that all of the sophisticated readers of this news group understand that the sharp corner of the square wave is composed of ever higher frequency waves. I'm even convinced most of them would not call this DC too. We agree on this. We would complicate the concept and thereby begin to confuse people if we insisted on using the "Stepped Wave" term. They would've been confused anyway. They don't seem to be confused, once the limitations of human language are overcome. We have many very intelligent and astute observers in this newsgroup. It is a simple step to recognize that if we can make a wave front with one battery, we can use a lot of batteries and carefully place and switch them to form a sine wave. The more batteries and switches, the better the representation. And this is still DC? Do you really know that mother nature is not ALWAYS operating in small steps of DC? How small is the scale that you can resolve to? I can not answer where DC starts and stops. Maybe you can? Is there some harm in considering Zo = 1/cC? This is best left in the privacy of the home. It seems that a simple yes or no answer could suffice here. How is "privacy in the home" related to Zo = 1/cC? However, none of your comments respond to the question: What is with this death grip on DC? What makes it so important that it be so tightly wedded to Waves? What mystery of the cosmos is answered with this union that has so long escaped the notice of centuries of trained thought? 73's Richard Clark, KB7QHC Please elaborate about the "death grip on DC". How is DC related to waves, or better, where does DC stop and waves begin? Should we never consider any portion of a wave to be DC like we do in calculus routinely? My original remark about about Zo = 1/cC expressed my surprise that such a relationship existed. It was not an original discovery by me, only new knowledge to me. From your reaction, this must be the first time you have run across the equation and how it might be derived. I provided two links to web pages where others have derived the equation from a different aspect, and even more pathways exist. It seems to be a very fundamental relationship despite being not well known or wide used. 73, Roger, W7WKB |
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