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Standing-Wave Current vs Traveling-Wave Current
Art wrote:
"So I added a time varient to a static field which provided a direct connection to Maxwell`s laws." It is said that Maxwell began with Faraday`s law of electromagnetic induction, which seems reasonable, as the voltage in one loop of wire inductively coupled to another is proportional to the derivative dphi/dt of current produced magnetic flux from the primary loop. Induced voltage does not arise at a single point on the loop but is the sum of all the infinitesimal bits of voltage distributed around the loop. Maxwell developed his first field equation from this start. Faraday`s law already deals with a time varying current to obtain induction. Different derivations are possible but Maxwell`s equations can express all known electromagnetic conditions at once. Oliver Heaviside made it his job to study Maxwell`s "Electromagnetic Theory", learn its mathematics, and reduce it to vector analysis. Heaviside published his results beginning a series of papers in 1887 in a British publication, "The Electrician", in a very understandable way. This has been called the start of modern communication engineering. Art also wrote: "The result for equilibrium must be a tank circuit where all energy is interchanged between the energy storage tanks (inductance and capacitance)" True that an EM wave exchanges its energy between an electric field and a magnetic field. Not true that a tank circuit type antenna is needed to launch or capture EM waves. An isolated wire, resonant or non-resonant is all that`s needed if it carries alternating current. Nor are explosives needed to generate radio waves. Less disruptive methods are quite acceptable. Art also wrote: "The bottom line is that for best efficiency for the unit volune supplied to an array must be in equilibrium." The above doesn`t square with what I`ve seen. Efficiency is output over input. Antenna efficiency is usually Radiation Resistance / Radiation Resistance + Loss Resistance. For the most antenna for the money, Terman suggests the Yagi or the Corner Reflector. Enough debunking for tonight. Best regards, Richard Harrison, KB5WZI |
Standing-Wave Current vs Traveling-Wave Current
"Richard Harrison" wrote in message ... Art wrote: "So I added a time varient to a static field which provided a direct connection to Maxwell`s laws." It is said that Maxwell began with Faraday`s law of electromagnetic can we do this... Maxwell did not write 'laws'. all of my references refer to "Maxwell's equations". Maxwell collected laws from Faraday, Gauss, Ohm, Ampere, and probably a few others and as far as I know added just the displacement current concept to turn them into a concise description of time varying electromagnetic phenomenon that has never been disproved. This set of equations is indeed what all antenna, feedline, waveguide, motors, power transmission, and related electromagnetic phenomenon are modeled with successfully in all environments that we have experienced. (neglecting things like black holes anyway) This includes diamagnetic, paramagnetic, ferromagnetic, insulators, conductors, dielectrics, and even the new man made negative refractive index materials. it is not necessary to add a new 'time varient' part to any of Maxwell's equations, they already contain all the time variant parts that are needed to explain any electromagnetic fields you can come up with. |
Standing-Wave Current vs Traveling-Wave Current
"Keith Dysart" wrote in message ... Thanks for offering the two capacitor/one capacitor view of the middle of the line. It took a bit of time to decide whether the commingling of the charge in the single capacitor at the middle of the line would solve my dilemma. So I considered this one capacitor in the exact center of a perfect transmission line. It is the perfect capacitor, absolutely symmetrical. So as the exactly equal currents flow into it on the exactly symmetrical leads, the charge is perfectly balanced so that the charge coming from each side exactly occupies its side of the conductor. As the two flows of charge flow over the perfectly symmetrical plates, they meet in the exact center, and flow no more. I conclude that a surface can be found exactly in the center of this capacitor across which no charge flows. Thus (un)happily returning me exactly to where I was before; there is a line across which no charge, and hence no energy, flows. absolutely correct. no charge flows through the insulator of a capacitor. you don't have to try hard to set up this condition, it is true of any capacitor that has no resistive losses. the concept you are struggling with is called the 'displacement current'. This is the unique concept that Maxwell added to the laws of Gauss, Faraday, et al when he compiled his set of electromagnetic equations. once you understand that then all will become clear. 2. I don't understand the mechanism which causes waves to bounce. I take this to imply that you are not happy with the simple "like charge repels"? waves do not bounce. waves superimpose on each other, but the original waves that meet in a homogenious, linear medium DO NOT INTERACT in any way. they each proceed happily on their way without any change. it is only due to the limited capability of your measurement instruments to measure the superimposed field that results that causes the confusion. if you could easily separate out the forward and reflected waves it would become intuitively obvious... however the poor instruments (swr meters and other 'power' meters) that have caused the confusion and resulted in the misnomer 'standing wave'. It is of course not a 'wave', nor does it 'stand'... it is just the result of superposition of 2 waves traveling in opposite directions. So the (poorly developped) "charge bouncing" explanation seems like a way out, but I certainly would appreciate other explanations for consideration. you don't need a 'way out' you need to go back to basics and learn the proper explanation. A large part of the argument seems to revolve around a single point in a perfect transmission line, where the current is exactly zero. This is an infinitesimal point on a perfect line, so some anomalous things might be expected to happen there. but the current, or voltage, is only zero because of the superimposed oppositely traveling waves. it is only your poor measurement instrument that only responds to the superimposed waves that causes the confusion. there. that ought to cause enough controversy to push this thread over the 1000 mark pretty quick! the wx is bad and i needed something to do today anyway since i can't go out and work on my maxwell compliant antennas. |
Standing-Wave Current vs Traveling-Wave Current
On 11 Jan, 05:00, "Dave" wrote:
"Richard Harrison" wrote in message ... Art wrote: "So I added a time varient to a static field which provided a direct connection to Maxwell`s laws." It is said that Maxwell began with Faraday`s law *of electromagnetic can we do this... Maxwell did not write 'laws'. *all of my references refer to "Maxwell's equations". *Maxwell collected laws from Faraday, Gauss, Ohm, Ampere, and probably a few others and as far as I know added just the displacement current concept to turn them into a concise description of time varying electromagnetic phenomenon that has never been disproved. *This set of equations is indeed what all antenna, feedline, waveguide, motors, power transmission, and related electromagnetic phenomenon are modeled with successfully in all environments that we have experienced. *(neglecting things like black holes anyway) *This includes diamagnetic, paramagnetic, ferromagnetic, insulators, conductors, dielectrics, and even the new man made negative refractive index materials. *it is not necessary to add a new 'time varient' part to any of Maxwell's equations, they already contain all the time variant parts that are needed to explain any electromagnetic fields you can come up with. I added a time varient to GAUSSIAN law to make it the same as Maxwellian laws, not the other way around as you are inferring. Before Maxwell came a long there were multiple laws stated many different ways. Maxwell saw that many of these laws tho written differently condensed to the same thing. So he condensed these multiple laws to a few but an no time did debunk the laws that already were in situ. All of these multiple laws as with Maxwell were built on the shoulders of Newton and those that contributed before him, all of which are derived around the pivot of gravity and equilibrium |
Standing-Wave Current vs Traveling-Wave Current
On Thu, 10 Jan 2008 18:52:28 -0800 (PST)
Keith Dysart wrote: snip............ I would really appreciate seeing some other possible explanations. One other one which I have seen and am not confortable with is the explanation that energy in the waves pass through the point in each direction and sum to zero. But this is indistinguishable from superposing power which most agree is inappropriate. As well, this explanation means that P(t) is not equal to V(t) times I(t), something that I am quite reluctant to agree with. The other explanation seen is that the voltage waves or the current waves travel down the line superpose, yielding a total voltage and current function at each point on the line which can be used to compute the power. With this explanation, P(t) is definitely equal to V(t) time I(t), which I do appreciate. The weakness of this explanation is that it seems to deny that the wave moves energy. And yet before the pulses collide it is easy to observe the energy moving in the line, and if a pulse was not coming in the other direction, there would be no dispute that the energy travelled to the end of the line and was absorbed in the load. Yet when the pulses collide, no energy crosses the middle of the line. Yet energy can be observed travelling in the line before and after the pulses collide. So... I can give up on pulses (or waves) moving energy. I am not happy doing that. I can give up on P(t) = V(t) * I(t). I am not happy doing that either. So the (poorly developped) "charge bouncing" explanation seems like a way out, but I certainly would appreciate other explanations for consideration. Hi Keith, I think you are putting too much emphasis on the measurement of energy in the pulse, or maybe not enought, depending upon how you are making and using the measurements. I hope you agree that the transmission line you are pulsing has no standing waves. If not, then the pulse must be a treveling wave. If it is a traveling wave, the impedance of the wave will be the impedance of the transmission line, except where the two pulses cross paths. At the crossing point, the impedance will jump to infinity, Z = v/i = v/zero = infinity. How about the energy/power levels? Except at the center, as the pulse passes, current and voltage can be measured, so power is being delivered from one section of the line to a second section more distant from the source. The energy delivered by the power equation can be measured by U = (v^2)/r = (i^2)*r where r is the Zo if the transmission line. Where the two pulses cross, the energy level must be the sum of the two energy levels, which would be 2U = 2*(v^2)/r (assuming two pulses of equal voltage). As you have pointed out, power would not flow at the point of wave first meeting, spreading from the meeting point back towards the two sources a distance equal to the square pulse width. Energy is present however, measured as U = (v^2)/r. The transmission line can be considered as a lineal capacitor, so U = (CV^2)/2, where C is the capacitance per unit length. If the waves "bounce", and occupy physical space for a period of time, they should comingle, stop, and fill the capacitor during that time. If so, 2U = C*V'^2 = 2*(V^2)/r where v is the voltage of a single pulse and V' = 1,414*v = voltage observed at point of crossing. At a disconinuity, we find a doubling of the voltages, not an increase of 1.414. This leads me to believe that the crossing pulses never stop in a physical sense. They do stop in the sense that power is not delived through the center point. 73, Roger, W7WKB |
Standing-Wave Current vs Traveling-Wave Current
On 11 Jan, 08:15, Roger Sparks wrote:
On Thu, 10 Jan 2008 18:52:28 -0800 (PST)Keith Dysart wrote: snip............ I would really appreciate seeing some other possible explanations. One other one which I have seen and am not confortable with is the explanation that energy in the waves pass through the point in each direction and sum to zero. But this is indistinguishable from superposing power which most agree is inappropriate. As well, this explanation means that P(t) is not equal to V(t) times I(t), something that I am quite reluctant to agree with. The other explanation seen is that the voltage waves or the current waves travel down the line superpose, yielding a total voltage and current function at each point on the line which can be used to compute the power. With this explanation, P(t) is definitely equal to V(t) time I(t), which I do appreciate. The weakness of this explanation is that it seems to deny that the wave moves energy. And yet before the pulses collide it is easy to observe the energy moving in the line, and if a pulse was not coming in the other direction, there would be no dispute that the energy travelled to the end of the line and was absorbed in the load. Yet when the pulses collide, no energy crosses the middle of the line. Yet energy can be observed travelling in the line before and after the pulses collide. So... I can give up on pulses (or waves) moving energy. I am not happy doing that. I can give up on P(t) = V(t) * I(t). I am not happy doing that either. So the (poorly developped) "charge bouncing" explanation seems like a way out, but I certainly would appreciate other explanations for consideration. Hi Keith, I think you are putting too much emphasis on the measurement of energy in the pulse, or maybe not enought, depending upon how you are making and using the measurements. * I hope you agree that the transmission line you are pulsing has no standing waves. *If not, then the pulse must be a treveling wave. *If it is a traveling wave, the impedance of the wave will be the impedance of the transmission line, except where the two pulses cross paths. *At the crossing point, the impedance will jump to infinity, Z = v/i = v/zero = infinity. How about the energy/power levels? *Except at the center, as the pulse passes, current and voltage can be measured, so power is being delivered from one section of the line to a second section more distant from the source. *The energy delivered by the power equation can be measured by U = (v^2)/r = (i^2)*r where r is the Zo if the transmission line. Where the two pulses cross, the energy level must be the sum of the two energy levels, which would be 2U = 2*(v^2)/r (assuming two pulses of equal voltage). *As you have pointed out, power would not flow at the point of wave first meeting, spreading from the meeting point back towards the two sources a distance equal to the square pulse width. Energy is present however, measured as U = (v^2)/r. The transmission line can be considered as a lineal capacitor, so U = (CV^2)/2, where C is the capacitance per unit length. *If the waves "bounce", and occupy physical space for a period of time, they should comingle, stop, and fill the capacitor during that time. If so, 2U = C*V'^2 * *= 2*(V^2)/r where v is the voltage of a single pulse and V' = 1,414*v = voltage observed at point of crossing. * At a disconinuity, we find a doubling of the voltages, not an increase of 1.414. *This leads me to believe that the crossing pulses never stop in a physical sense. *They do stop in the sense that power is not delived through the center point. 73, Roger, W7WKB- Hide quoted text - - Show quoted text - Roger you are conversing with old men most of which oppose change. Having been taught some fifty years ago they want to protect those teachings the originators of which are all dead. Thus regardless of what has happened and discovered or intruded upon by inquiring minds they wish to stay in the past.In the past, statics was viewed as a subset of electro-dynamics and the old timers want it to stay that way. By starting with Gauss and adding a time varient I added a visual to Maxwell that was missing from his equations because Gauss was not the leading contributor to the time varient theme. It is this that the old timers are resisting because it brings away the thought that statics is just a subset. Thus you see that there is inherrent resistance to the mathematics that supplies a visual to Mawellian equations. It took Richard several months to accept the legitimacy of the mathematics involved in the steps I took. As yet nobody else has admitted to the legitamacy of the mathematics. Thus protecting the notion of static being just a subset. This manoever has placed ham radio into a quagmire from which they cannot extricate themselves and thus advance to analyse the intricacies of propagation. Who would have believed that ham radio would take to task of a Doctor working at MIT on space reseach for NASA for faulty use of mathematics to prove the relavence of statics? Can science really be held up while old men are still living? Art Unwin KB9MZ...XG |
Standing-Wave Current vs Traveling-Wave Current
roger chimed in with:
I hope you agree that the transmission line you are pulsing has no standing waves. If not, then the pulse must be a treveling wave. If it is a traveling wave, the impedance of the wave will be the impedance of the transmission line, except where the two pulses cross paths. At the crossing point, the impedance will jump to infinity, Z = v/i = v/zero = infinity. argh, another misconception!.. the impedance of a transmission line doesn't change! and the impedance seen by a single traveling wave never changes either. the measured ratio of voltage to current at a point on the line can change as a result of the superposition of traveling waves. but again, that is just a result of cheap instrumentation that can't resolve the component waves. |
Standing-Wave Current vs Traveling-Wave Current
On Fri, 11 Jan 2008 08:15:09 -0800, Roger Sparks
wrote: They do stop in the sense that power is not delived through the center point. Hi Roger, I'm not sure if this is original to you, or one of those conceits that is being passed around; but how, short of tagging energy (power?), can you tell its origin? In other words, delivery by return, or completion of the path needs to be separable by some information about the origin that to this point has been missing from the discussion. If energy can be tagged with a return address, what is that tag? 73's Richard Clark, KB7QHC |
Standing-Wave Current vs Traveling-Wave Current
On Fri, 11 Jan 2008 17:19:28 GMT
"Dave" wrote: roger chimed in with: I hope you agree that the transmission line you are pulsing has no standing waves. If not, then the pulse must be a treveling wave. If it is a traveling wave, the impedance of the wave will be the impedance of the transmission line, except where the two pulses cross paths. At the crossing point, the impedance will jump to infinity, Z = v/i = v/zero = infinity. argh, another misconception!.. the impedance of a transmission line doesn't change! and the impedance seen by a single traveling wave never changes either. the measured ratio of voltage to current at a point on the line can change as a result of the superposition of traveling waves. but again, that is just a result of cheap instrumentation that can't resolve the component waves. Good point. It would have been much better to say something like :"At the crossing point, the MEASURED impedance will jump to infinity (Z = v/i = v/zero = infinity) but we have no indication that the impedance of either the wire or the individual pulse changes in any way.". 73, Roger, W7WKB |
Standing-Wave Current vs Traveling-Wave Current
On Fri, 11 Jan 2008 10:44:19 -0800
Richard Clark wrote: On Fri, 11 Jan 2008 08:15:09 -0800, Roger Sparks wrote: They do stop in the sense that power is not delived through the center point. Hi Roger, I'm not sure if this is original to you, or one of those conceits that is being passed around; but how, short of tagging energy (power?), can you tell its origin? In other words, delivery by return, or completion of the path needs to be separable by some information about the origin that to this point has been missing from the discussion. If energy can be tagged with a return address, what is that tag? 73's Richard Clark, KB7QHC Current is the tag, and the address is "past" and "future". Measurement is always "present", but we like to make predictions about what will happen in the future, and trace what has happened in the past. With the electromagnetic equations, we are quite good at making those extrapolations from present measurements. At the crossing point, we can not measure current, so the power equation of P = V * I fails. There is no power at this point that we can measure. We can measure instantaneous voltage but don't know which equation to use to determine energy, U = (CV^2)/2 or SumU = Sum((V^2)/r). Only if we make many measurements over time can we learn the shape of the voltage over time, and thereby deduce which equation to use. 73, Roger, W7WKB At the crossing poiont |
Standing-Wave Current vs Traveling-Wave Current
On Fri, 11 Jan 2008 11:45:10 -0800, Roger Sparks
wrote: Current is the tag .... At the crossing point, we can not measure current, Hi Roger, Hence the information as to the source of energy that arrives at its final destination is completely lost. Barring this tracking, then, there is no way to prove effects due to the "crossing point." So, why does this discussion proceed without hope of any meaningful proof? Certainly, given more than 400, 500, 1000 postings there must be some other tagging mechanism that you are unaware of, or has been withheld from comment. Did we miss that announcement? 73's Richard Clark, KB7QHC |
Standing-Wave Current vs Traveling-Wave Current
On Fri, 11 Jan 2008 08:44:01 -0800 (PST)
art wrote: Roger you are conversing with old men most of which oppose change. Having been taught some fifty years ago they want to protect those teachings the originators of which are all dead. Thus regardless of what has happened and discovered or intruded upon by inquiring minds they wish to stay in the past.In the past, statics was viewed as a subset of electro-dynamics and the old timers want it to stay that way. By starting with Gauss and adding a time varient I added a visual to Maxwell that was missing from his equations because Gauss was not the leading contributor to the time varient theme. It is this that the old timers are resisting because it brings away the thought that statics is just a subset. Thus you see that there is inherrent resistance to the mathematics that supplies a visual to Mawellian equations. It took Richard several months to accept the legitimacy of the mathematics involved in the steps I took. As yet nobody else has admitted to the legitamacy of the mathematics. Thus protecting the notion of static being just a subset. This manoever has placed ham radio into a quagmire from which they cannot extricate themselves and thus advance to analyse the intricacies of propagation. Who would have believed that ham radio would take to task of a Doctor working at MIT on space reseach for NASA for faulty use of mathematics to prove the relavence of statics? Can science really be held up while old men are still living? Art Unwin KB9MZ...XG Hi Art, Like you, I would like to find a better way of doing things, especially some easier math for the electromagnetic equations. Until we find that better way, we must use what we have. What we have is very, very good, because it has brought us TV, computers, the Internet, space travel, and much more. What ever we find that could be "better", must also contain the knowledge we have today, but perhaps can explain todays knowledge easier or more completely. I try to learn from the old men because the sum of their knowledge is far greater than my own can ever be. Having said that, I also recognize that the knowledge of each man is limited by his own talent, experience, and human frailty, so a judgement must be made as to wisdom and accuracy. I really admire the willingness of all participants to contribute to discussions. The hard part is knowing how to fit each new tibit of knowledge into my own personal knowledge base. 73, Roger, W7WKB |
Standing-Wave Current vs Traveling-Wave Current
On Fri, 11 Jan 2008 11:59:24 -0800
Richard Clark wrote: So, why does this discussion proceed without hope of any meaningful proof? Certainly, given more than 400, 500, 1000 postings there must be some other tagging mechanism that you are unaware of, or has been withheld from comment. Did we miss that announcement? 73's Richard Clark, KB7QHC The writtings of many of us still have "hope". Many postings reflect a curiosity that has not been satisfied. Is there a tagging mechanism that I did not mention? If so, please articulate it. 73, Roger, W7WKB |
Standing-Wave Current vs Traveling-Wave Current
On Fri, 11 Jan 2008 12:23:39 -0800, Roger Sparks
wrote: The writtings of many of us still have "hope". Hi Roger, Ah, yes. Hope without proof is called faith. There are testimonials, and there are witnesses to miracles - however, those, too, seem to be far and few between. Faith in "what" seems to be an even greater mystery, and a strange basis for belief. Another conceit I've seen ripple through the threads - I don't think you offered it either, but authorship is vague - is that this "what" may be waves bouncing. Hope in waves bouncing (for which only faith supports this where proof is absent) may solve the mystery of "what," but like Russian Dolls nested one inside another, certainly this faith is ever spiraling out toward some even greater mystery in beliefs. To put it in religious terms: "So What?" Is this the road to redemption? Is it like the discovery of the mirror? Did the discoverer (inventor if you will seeing as the mirror might be currently in the process of patenting) attain a new insight? a new perspective? Even there, our using (measuring with) a mirror gives us a means to tag information through parallax. Is this thread missing something as simple as parallax to tag currents as to their origin? It would seem after 800 contributions that this contribution (parallax) would have resolved the thread and brought closure to allow everyone to transcend obstacles on that road to redemption. Is anyone actually pursuing the goal of finding and expressing the parallax problem (or revealing any tagging); or are they simply content to have hope and wait for the end of days milling about the edges of the purgatory of Babel? 73's Richard Clark, KB7QHC |
Standing-Wave Current vs Traveling-Wave Current
On Jan 11, 8:12*am, "Dave" wrote:
"Keith Dysart" wrote in message ... Thanks for offering the two capacitor/one capacitor view of the middle of the line. It took a bit of time to decide whether the commingling of the charge in the single capacitor at the middle of the line would solve my dilemma. So I considered this one capacitor in the exact center of a perfect transmission line. It is the perfect capacitor, absolutely symmetrical. So as the exactly equal currents flow into it on the exactly symmetrical leads, the charge is perfectly balanced so that the charge coming from each side exactly occupies its side of the conductor. As the two flows of charge flow over the perfectly symmetrical plates, they meet in the exact center, and flow no more. I conclude that a surface can be found *exactly in the center of this capacitor across which no charge flows. Thus (un)happily returning me exactly to where I was before; there is a line across which no charge, and hence no energy, flows. absolutely correct. *no charge flows through the insulator of a capacitor. |
Standing-Wave Current vs Traveling-Wave Current
On Jan 11, 11:15*am, Roger Sparks wrote:
On Thu, 10 Jan 2008 18:52:28 -0800 (PST)Keith Dysart wrote: snip............ I would really appreciate seeing some other possible explanations. One other one which I have seen and am not confortable with is the explanation that energy in the waves pass through the point in each direction and sum to zero. But this is indistinguishable from superposing power which most agree is inappropriate. As well, this explanation means that P(t) is not equal to V(t) times I(t), something that I am quite reluctant to agree with. The other explanation seen is that the voltage waves or the current waves travel down the line superpose, yielding a total voltage and current function at each point on the line which can be used to compute the power. With this explanation, P(t) is definitely equal to V(t) time I(t), which I do appreciate. The weakness of this explanation is that it seems to deny that the wave moves energy. And yet before the pulses collide it is easy to observe the energy moving in the line, and if a pulse was not coming in the other direction, there would be no dispute that the energy travelled to the end of the line and was absorbed in the load. Yet when the pulses collide, no energy crosses the middle of the line. Yet energy can be observed travelling in the line before and after the pulses collide. So... I can give up on pulses (or waves) moving energy. I am not happy doing that. I can give up on P(t) = V(t) * I(t). I am not happy doing that either. So the (poorly developped) "charge bouncing" explanation seems like a way out, but I certainly would appreciate other explanations for consideration. Hi Keith, I think you are putting too much emphasis on the measurement of energy in the pulse, or maybe not enought, depending upon how you are making and using the measurements. * I hope you agree that the transmission line you are pulsing has no standing waves. * "Standing waves" seem to more be a consequence of sinusoidal excitation than pulse. So I expect no "standing waves". I don't even like using the words "traveling wave" to describe the pulse situation since "traveling wave" also seems to bring a lot of baggage. If not, then the pulse must be a treveling wave. *If it is a traveling wave, the impedance of the wave will be the impedance of the transmission line, except where the two pulses cross paths. *At the crossing point, the impedance will jump to infinity, Z = v/i = v/zero = infinity. I do not recommend computing this ratio and calling it impedance. I find it leads to difficulties. Better just to think of the V and I independantly. How about the energy/power levels? *Except at the center, as the pulse passes, current and voltage can be measured, so power is being delivered from one section of the line to a second section more distant from the source. *The energy delivered by the power equation can be measured by U = (v^2)/r = (i^2)*r where r is the Zo if the transmission line. More accurately P(t) = V(t) * I(t). it happens that for the pulses in question, except when colliding, that V and I of the pulses observed on the line are related by Z0 so by substitution, the expressions above can be derived. But sometimes it is better to stick with the more basic expression P=VI. Where the two pulses cross, the energy level must be the sum of the two energy levels, which would be 2U = 2*(v^2)/r (assuming two pulses of equal voltage). *As you have pointed out, power would not flow at the point of wave first meeting, spreading from the meeting point back towards the two sources a distance equal to the square pulse width. Energy is present however, measured as U = (v^2)/r. The transmission line can be considered as a lineal capacitor, so U = (CV^2)/2, where C is the capacitance per unit length. *If the waves "bounce", and occupy physical space for a period of time, they should comingle, stop, and fill the capacitor during that time. If so, 2U = C*V'^2 * *= 2*(V^2)/r where v is the voltage of a single pulse and V' = 1,414*v = voltage observed at point of crossing. * But the voltage at the crossing is 2V. A puzzle? When the pulse is "travelling", there is energy in the capacitance and in the inductance of the line. When the current stops, the energy in the inductance is added to the energy in the capacitance, thus the voltage reaches 2V. At a disconinuity, we find a doubling of the voltages, not an increase of 1.414. *This leads me to believe that the crossing pulses never stop in a physical sense. *They do stop in the sense that power is not delived through the center point. ...Keith |
Standing-Wave Current vs Traveling-Wave Current
On Jan 11, 1:44*pm, Richard Clark wrote:
On Fri, 11 Jan 2008 08:15:09 -0800, Roger Sparks wrote: They do stop in the sense that power is not delived through the center point. Hi Roger, I'm not sure if this is original to you, or one of those conceits that is being passed around; but how, short of tagging energy (power?), can you tell its origin? *In other words, delivery by return, or completion of the path needs to be separable by some information about the origin that to this point has been missing from the discussion. If energy can be tagged with a return address, what is that tag? I suggest that since the current at the middle of the line is always 0, the power is always 0 and therefore no energy crosses the middle. While tracking mixed energy is difficult, when no energy crosses a boundary it seems easy to keep the energy on each side of the boundary separate. ...Keith |
Standing-Wave Current vs Traveling-Wave Current
"Keith Dysart" wrote in message ... absolutely correct. no charge flows through the insulator of a capacitor. This was not the line I meant. My line was perpendicular to the plates. Current does not cross this line because it arrives equally from both sides. huh?? no charge passes from one plate of a capacitor to the other. but current does in the form of displacement current. if you are trying to look at the microscopic field and charge distributions during a transient in a capacitor you are way beyond anything i ever studied, or would want to study. waves do not bounce. What about charge? charge is being moved by the fields of the wave, and it moves very little in the wire as has been shown in the past. when equal and opposite waves arrived at a point where the current cancels the charges superimpose to result in a zero field so there is no motion, hence no current at that point. as the waves pass each other the fields no longer cancel so the electrons on the other side of the cancelation point start to move again in the opposite directions. if you want to call that a bounce knock yourself out, but it will lead to a rather limited view that is only helpful in certain circumstances where exact cancelation occurs. Or is it the "standing wave" which is real and it just happens that it can also be described as the sum of two waves going in opposite directions? But the wave going in one direction can be described as the sum of a number of waves going in that direction? (Especially\ when there are multiple reflections!) How many waves in each direction? When do we stop? I respectfully submit that it is only the resultant that is real. The rest are merely alternate descriptions (though often useful). then enjoy your fantasy. the forward and reverse wave components are easily separated and observed anywhere on the line. its just that most amateur grade equipment doesn't bother because it is sufficient for 99.44% of us to only measure your 'real' standing wave to properly adjust our antennas and radios. |
Standing-Wave Current vs Traveling-Wave Current
On Fri, 11 Jan 2008 14:03:10 -0800 (PST), Keith Dysart
wrote: On Jan 11, 1:44*pm, Richard Clark wrote: On Fri, 11 Jan 2008 08:15:09 -0800, Roger Sparks wrote: They do stop in the sense that power is not delived through the center point. Hi Roger, I'm not sure if this is original to you, or one of those conceits that is being passed around; but how, short of tagging energy (power?), can you tell its origin? *In other words, delivery by return, or completion of the path needs to be separable by some information about the origin that to this point has been missing from the discussion. If energy can be tagged with a return address, what is that tag? I suggest that since the current at the middle of the line is always 0, the power is always 0 and therefore no energy crosses the middle. While tracking mixed energy is difficult, when no energy crosses a boundary it seems easy to keep the energy on each side of the boundary separate. Hi Keith, If you cannot identify the source, then you cannot proclaim a separation. The best term for this is "the enigma effect." I hate to turn this loose on the world because I know many here will pick it up and run to their perceived goal for a touch-down. Before anyone tackles me for a touchback, I'm going to pass this off and watch the quarterbacks wrestle with religion in the huddle. 73's Richard Clark, KB7QHC |
Standing-Wave Current vs Traveling-Wave Current
On 11 Jan, 14:03, Keith Dysart wrote:
On Jan 11, 1:44*pm, Richard Clark wrote: On Fri, 11 Jan 2008 08:15:09 -0800, Roger Sparks wrote: They do stop in the sense that power is not delived through the center point. Hi Roger, I'm not sure if this is original to you, or one of those conceits that is being passed around; but how, short of tagging energy (power?), can you tell its origin? *In other words, delivery by return, or completion of the path needs to be separable by some information about the origin that to this point has been missing from the discussion. If energy can be tagged with a return address, what is that tag? I suggest that since the current at the middle of the line is always 0, the power is always 0 and therefore no energy crosses the middle. While tracking mixed energy is difficult, when no energy crosses a boundary it seems easy to keep the energy on each side of the boundary separate. ...Keith Keith, Richard has not entered the actual discussion nor has he shown any indication he understands what is going on. All he is doing is intimating he knows all the answers but he is not going to reveal them. Why? He has no choice if later he wants to state "I knew that all the time". In the mean time he is taunting people with off subject topics and then deigns not to provide technical content. He is very good at arousing people to respond to him in a defensive manner as you can now personally point out, usually by asking questions without any effort to support the discussion.His degree is in english which is why he is practicing on this newsgroup Have a great week end Art |
Standing-Wave Current vs Traveling-Wave Current
On Jan 11, 5:03 pm, Keith Dysart wrote:
I suggest that since the current at the middle of the line is always 0, the power is always 0 and therefore no energy crosses the middle. While tracking mixed energy is difficult, when no energy crosses a boundary it seems easy to keep the energy on each side of the boundary separate. Of course, what you say is only true for net energy. If we have a forward Poynting vector of 100 watts and a reflected Poynting vector of 100 watts, no net energy is flowing at any point. -- 73, Cecil, w5dxp.com |
Standing-Wave Current vs Traveling-Wave Current
Richard Clark wrote: On Fri, 11 Jan 2008 14:03:10 -0800 (PST), Keith Dysart wrote: On Jan 11, 1:44 pm, Richard Clark wrote: On Fri, 11 Jan 2008 08:15:09 -0800, Roger Sparks wrote: They do stop in the sense that power is not delived through the center point. Hi Roger, I'm not sure if this is original to you, or one of those conceits that is being passed around; but how, short of tagging energy (power?), can you tell its origin? In other words, delivery by return, or completion of the path needs to be separable by some information about the origin that to this point has been missing from the discussion. If energy can be tagged with a return address, what is that tag? I suggest that since the current at the middle of the line is always 0, the power is always 0 and therefore no energy crosses the middle. While tracking mixed energy is difficult, when no energy crosses a boundary it seems easy to keep the energy on each side of the boundary separate. Hi Keith, If you cannot identify the source, then you cannot proclaim a separation. The best term for this is "the enigma effect." I hate to turn this loose on the world because I know many here will pick it up and run to their perceived goal for a touch-down. Before anyone tackles me for a touchback, I'm going to pass this off and watch the quarterbacks wrestle with religion in the huddle. 73's Richard Clark, KB7QHC To single out a particular spot as the site of a lack of energy movement along an equipotential system in which there is no tranfer of energy anyway seems to me to be an arbitrary convenience. Maxwell explained how electromagentic waves 'bounce' if they encounter matter, and I haven't seen any evidence that it was an incomplete description. ac6xg |
Standing-Wave Current vs Traveling-Wave Current
On Fri, 11 Jan 2008 13:59:47 -0800 (PST)
Keith Dysart wrote: On Jan 11, 11:15*am, Roger Sparks wrote: On Thu, 10 Jan 2008 18:52:28 -0800 (PST)Keith Dysart wrote: snip............ I would really appreciate seeing some other possible explanations. One other one which I have seen and am not confortable with is the explanation that energy in the waves pass through the point in each direction and sum to zero. But this is indistinguishable from superposing power which most agree is inappropriate. As well, this explanation means that P(t) is not equal to V(t) times I(t), something that I am quite reluctant to agree with. The other explanation seen is that the voltage waves or the current waves travel down the line superpose, yielding a total voltage and current function at each point on the line which can be used to compute the power. With this explanation, P(t) is definitely equal to V(t) time I(t), which I do appreciate. The weakness of this explanation is that it seems to deny that the wave moves energy. And yet before the pulses collide it is easy to observe the energy moving in the line, and if a pulse was not coming in the other direction, there would be no dispute that the energy travelled to the end of the line and was absorbed in the load. Yet when the pulses collide, no energy crosses the middle of the line. Yet energy can be observed travelling in the line before and after the pulses collide. So... I can give up on pulses (or waves) moving energy. I am not happy doing that. I can give up on P(t) = V(t) * I(t). I am not happy doing that either. So the (poorly developped) "charge bouncing" explanation seems like a way out, but I certainly would appreciate other explanations for consideration. Hi Keith, I think you are putting too much emphasis on the measurement of energy in the pulse, or maybe not enought, depending upon how you are making and using the measurements. * I hope you agree that the transmission line you are pulsing has no standing waves. * "Standing waves" seem to more be a consequence of sinusoidal excitation than pulse. So I expect no "standing waves". I don't even like using the words "traveling wave" to describe the pulse situation since "traveling wave" also seems to bring a lot of baggage. If not, then the pulse must be a treveling wave. *If it is a traveling wave, the impedance of the wave will be the impedance of the transmission line, except where the two pulses cross paths. *At the crossing point, the impedance will jump to infinity, Z = v/i = v/zero = infinity. I do not recommend computing this ratio and calling it impedance. I find it leads to difficulties. Better just to think of the V and I independantly. How about the energy/power levels? *Except at the center, as the pulse passes, current and voltage can be measured, so power is being delivered from one section of the line to a second section more distant from the source. *The energy delivered by the power equation can be measured by U = (v^2)/r = (i^2)*r where r is the Zo if the transmission line. More accurately P(t) = V(t) * I(t). it happens that for the pulses in question, except when colliding, that V and I of the pulses observed on the line are related by Z0 so by substitution, the expressions above can be derived. But sometimes it is better to stick with the more basic expression P=VI. Where the two pulses cross, the energy level must be the sum of the two energy levels, which would be 2U = 2*(v^2)/r (assuming two pulses of equal voltage). *As you have pointed out, power would not flow at the point of wave first meeting, spreading from the meeting point back towards the two sources a distance equal to the square pulse width. Energy is present however, measured as U = (v^2)/r. The transmission line can be considered as a lineal capacitor, so U = (CV^2)/2, where C is the capacitance per unit length. *If the waves "bounce", and occupy physical space for a period of time, they should comingle, stop, and fill the capacitor during that time. If so, 2U = C*V'^2 * *= 2*(V^2)/r where v is the voltage of a single pulse and V' = 1,414*v = voltage observed at point of crossing. * But the voltage at the crossing is 2V. A puzzle? When the pulse is "travelling", there is energy in the capacitance and in the inductance of the line. When the current stops, the energy in the inductance is added to the energy in the capacitance, thus the voltage reaches 2V. Which is correct? P = (v^2)/r = (i^2)r or P = (v^2)/r + (i^2)r If P = (v^2)/r = (i^2)r is correct, what is the precondition that MUST be true? Answer: The i and v measurements must be across a pure resistance, without reactance. The traveling wave is considered to have a pure resistive impedance. This going by measurements makes things hard! Too bad we can't see and feel the wave with our own eyes and hands! At a disconinuity, we find a doubling of the voltages, not an increase of 1.414. *This leads me to believe that the crossing pulses never stop in a physical sense. *They do stop in the sense that power is not delived through the center point. ...Keith 73, Roger, W7WKB |
Standing-Wave Current vs Traveling-Wave Current
On Jan 11, 7:30*pm, Roger Sparks wrote:
On Fri, 11 Jan 2008 13:59:47 -0800 (PST) Keith Dysart wrote: On Jan 11, 11:15*am, Roger Sparks wrote: On Thu, 10 Jan 2008 18:52:28 -0800 (PST)Keith Dysart wrote: snip............ I would really appreciate seeing some other possible explanations. One other one which I have seen and am not confortable with is the explanation that energy in the waves pass through the point in each direction and sum to zero. But this is indistinguishable from superposing power which most agree is inappropriate. As well, this explanation means that P(t) is not equal to V(t) times I(t), something that I am quite reluctant to agree with. The other explanation seen is that the voltage waves or the current waves travel down the line superpose, yielding a total voltage and current function at each point on the line which can be used to compute the power. With this explanation, P(t) is definitely equal to V(t) time I(t), which I do appreciate. The weakness of this explanation is that it seems to deny that the wave moves energy. And yet before the pulses collide it is easy to observe the energy moving in the line, and if a pulse was not coming in the other direction, there would be no dispute that the energy travelled to the end of the line and was absorbed in the load. Yet when the pulses collide, no energy crosses the middle of the line. Yet energy can be observed travelling in the line before and after the pulses collide. So... I can give up on pulses (or waves) moving energy. I am not happy doing that. I can give up on P(t) = V(t) * I(t). I am not happy doing that either. So the (poorly developped) "charge bouncing" explanation seems like a way out, but I certainly would appreciate other explanations for consideration. Hi Keith, I think you are putting too much emphasis on the measurement of energy in the pulse, or maybe not enought, depending upon how you are making and using the measurements. * I hope you agree that the transmission line you are pulsing has no standing waves. * "Standing waves" seem to more be a consequence of sinusoidal excitation than pulse. So I expect no "standing waves". I don't even like using the words "traveling wave" to describe the pulse situation since "traveling wave" also seems to bring a lot of baggage. If not, then the pulse must be a treveling wave. *If it is a traveling wave, the impedance of the wave will be the impedance of the transmission line, except where the two pulses cross paths. *At the crossing point, the impedance will jump to infinity, Z = v/i = v/zero = infinity. I do not recommend computing this ratio and calling it impedance. I find it leads to difficulties. Better just to think of the V and I independantly. How about the energy/power levels? *Except at the center, as the pulse passes, current and voltage can be measured, so power is being delivered from one section of the line to a second section more distant from the source. *The energy delivered by the power equation can be measured by U = (v^2)/r = (i^2)*r where r is the Zo if the transmission line. More accurately P(t) = V(t) * I(t). it happens that for the pulses in question, except when colliding, that V and I of the pulses observed on the line are related by Z0 so by substitution, the expressions above can be derived. But sometimes it is better to stick with the more basic expression P=VI. Where the two pulses cross, the energy level must be the sum of the two energy levels, which would be 2U = 2*(v^2)/r (assuming two pulses of equal voltage). *As you have pointed out, power would not flow at the point of wave first meeting, spreading from the meeting point back towards the two sources a distance equal to the square pulse width. Energy is present however, measured as U = (v^2)/r. The transmission line can be considered as a lineal capacitor, so U = (CV^2)/2, where C is the capacitance per unit length. *If the waves "bounce", and occupy physical space for a period of time, they should comingle, stop, and fill the capacitor during that time. If so, 2U = C*V'^2 * *= 2*(V^2)/r where v is the voltage of a single pulse and V' = 1,414*v = voltage observed at point of crossing. * But the voltage at the crossing is 2V. A puzzle? When the pulse is "travelling", there is energy in the capacitance and in the inductance of the line. When the current stops, the energy in the inductance is added to the energy in the capacitance, thus the voltage reaches 2V. Which is correct? *P = (v^2)/r = (i^2)r * or * P = (v^2)/r + (i^2)r P(t) = V(t) * I(t) by substitution from V = I * R P(t) = V(t) * V(t) / R and P(t) = I(t) * I(t) * R But recall that power is the flow of energy per unit time. The energy present in any section of line is the energy present in the electric field of the capacitance plus the energy present in the magnetic field of the inductance. So from your expressions above U = (CV^2)/2 + (LI^2)/2 If P = (v^2)/r = (i^2)r is correct, what is the precondition that MUST be true? Answer: The i and v measurements must be across a pure resistance, without reactance. This is why it is often better just to use the original equation: P(t) = V(t) * I(t) for it is always true and requires no preconditions. The traveling wave is considered to have a pure resistive impedance. This going by measurements makes things hard! *Too bad we can't see and feel the wave with our own eyes and hands! At a disconinuity, we find a doubling of the voltages, not an increase of 1.414. *This leads me to believe that the crossing pulses never stop in a physical sense. *They do stop in the sense that power is not delived through the center point. ...Keith 73, Roger, W7WKB- Hide quoted text - ...Keith |
Standing-Wave Current vs Traveling-Wave Current
On Jan 11, 5:25*pm, Richard Clark wrote:
On Fri, 11 Jan 2008 14:03:10 -0800 (PST), Keith Dysart wrote: On Jan 11, 1:44*pm, Richard Clark wrote: On Fri, 11 Jan 2008 08:15:09 -0800, Roger Sparks wrote: They do stop in the sense that power is not delived through the center point. Hi Roger, I'm not sure if this is original to you, or one of those conceits that is being passed around; but how, short of tagging energy (power?), can you tell its origin? *In other words, delivery by return, or completion of the path needs to be separable by some information about the origin that to this point has been missing from the discussion. If energy can be tagged with a return address, what is that tag? I suggest that since the current at the middle of the line is always 0, the power is always 0 and therefore no energy crosses the middle. While tracking mixed energy is difficult, when no energy crosses a boundary it seems easy to keep the energy on each side of the boundary separate. Hi Keith, If you cannot identify the source, then you cannot proclaim a separation. That is hardly difficult. If no energy every crosses the middle of the line, then the energy on the left half of the line originated with the source on the left side and ditto for the right. ...Keith |
Standing-Wave Current vs Traveling-Wave Current
On Fri, 11 Jan 2008 18:51:07 -0800 (PST), Keith Dysart
wrote: If you cannot identify the source, then you cannot proclaim a separation. That is hardly difficult. If no energy every crosses the middle of the line, Hi Keith, If indeed. The difficulty is you've already allowed that the energy is not tagged, so its source is unknown at the load. So "if" fails through this immutable correlation. The separation is not demonstrated. 73's Richard Clark, KB7QHC |
Standing-Wave Current vs Traveling-Wave Current
On Jan 11, 6:56*pm, Cecil Moore wrote:
On Jan 11, 5:03 pm, Keith Dysart wrote: I suggest that since the current at the middle of the line is always 0, the power is always 0 and therefore no energy crosses the middle. While tracking mixed energy is difficult, when no energy crosses a boundary it seems easy to keep the energy on each side of the boundary separate. Of course, what you say is only true for net energy. If we have a forward Poynting vector of 100 watts and a reflected Poynting vector of 100 watts, no net energy is flowing at any point. You don't need Poynting vectors to realize that when the instantaneous power is always 0, no energy is flowing. And when the instantaneous power is always 0, it is unnecessary to integrate and average to compute the net energy flow, because no energy is flowing at all. And if by your response you really do mean that energy can be flowing when the instantaneous power is always 0, please be direct and say so. But then you will have to come up with a new definition of instantaneous power for it can not be that it is the rate of energy transfer if energy is flowing when the instantaneous power is zero. ...Keith |
Standing-Wave Current vs Traveling-Wave Current
On Fri, 11 Jan 2008 18:49:20 -0800 (PST)
Keith Dysart wrote: On Jan 11, 7:30*pm, Roger Sparks wrote: On Fri, 11 Jan 2008 13:59:47 -0800 (PST) Keith Dysart wrote: On Jan 11, 11:15*am, Roger Sparks wrote: On Thu, 10 Jan 2008 18:52:28 -0800 (PST)Keith Dysart wrote: snip............ I would really appreciate seeing some other possible explanations. One other one which I have seen and am not confortable with is the explanation that energy in the waves pass through the point in each direction and sum to zero. But this is indistinguishable from superposing power which most agree is inappropriate. As well, this explanation means that P(t) is not equal to V(t) times I(t), something that I am quite reluctant to agree with. The other explanation seen is that the voltage waves or the current waves travel down the line superpose, yielding a total voltage and current function at each point on the line which can be used to compute the power. With this explanation, P(t) is definitely equal to V(t) time I(t), which I do appreciate. The weakness of this explanation is that it seems to deny that the wave moves energy. And yet before the pulses collide it is easy to observe the energy moving in the line, and if a pulse was not coming in the other direction, there would be no dispute that the energy travelled to the end of the line and was absorbed in the load. Yet when the pulses collide, no energy crosses the middle of the line. Yet energy can be observed travelling in the line before and after the pulses collide. So... I can give up on pulses (or waves) moving energy. I am not happy doing that. I can give up on P(t) = V(t) * I(t). I am not happy doing that either. So the (poorly developped) "charge bouncing" explanation seems like a way out, but I certainly would appreciate other explanations for consideration. Hi Keith, I think you are putting too much emphasis on the measurement of energy in the pulse, or maybe not enought, depending upon how you are making and using the measurements. * I hope you agree that the transmission line you are pulsing has no standing waves. * "Standing waves" seem to more be a consequence of sinusoidal excitation than pulse. So I expect no "standing waves". I don't even like using the words "traveling wave" to describe the pulse situation since "traveling wave" also seems to bring a lot of baggage. If not, then the pulse must be a treveling wave. *If it is a traveling wave, the impedance of the wave will be the impedance of the transmission line, except where the two pulses cross paths. *At the crossing point, the impedance will jump to infinity, Z = v/i = v/zero = infinity. I do not recommend computing this ratio and calling it impedance. I find it leads to difficulties. Better just to think of the V and I independantly. How about the energy/power levels? *Except at the center, as the pulse passes, current and voltage can be measured, so power is being delivered from one section of the line to a second section more distant from the source. *The energy delivered by the power equation can be measured by U = (v^2)/r = (i^2)*r where r is the Zo if the transmission line. More accurately P(t) = V(t) * I(t). it happens that for the pulses in question, except when colliding, that V and I of the pulses observed on the line are related by Z0 so by substitution, the expressions above can be derived. But sometimes it is better to stick with the more basic expression P=VI. Where the two pulses cross, the energy level must be the sum of the two energy levels, which would be 2U = 2*(v^2)/r (assuming two pulses of equal voltage). *As you have pointed out, power would not flow at the point of wave first meeting, spreading from the meeting point back towards the two sources a distance equal to the square pulse width. Energy is present however, measured as U = (v^2)/r. The transmission line can be considered as a lineal capacitor, so U = (CV^2)/2, where C is the capacitance per unit length. *If the waves "bounce", and occupy physical space for a period of time, they should comingle, stop, and fill the capacitor during that time. If so, 2U = C*V'^2 * *= 2*(V^2)/r where v is the voltage of a single pulse and V' = 1,414*v = voltage observed at point of crossing. * But the voltage at the crossing is 2V. A puzzle? When the pulse is "travelling", there is energy in the capacitance and in the inductance of the line. When the current stops, the energy in the inductance is added to the energy in the capacitance, thus the voltage reaches 2V. Which is correct? *P = (v^2)/r = (i^2)r * or * P = (v^2)/r + (i^2)r P(t) = V(t) * I(t) by substitution from V = I * R P(t) = V(t) * V(t) / R and P(t) = I(t) * I(t) * R Correct. But recall that power is the flow of energy per unit time. The energy present in any section of line is the energy present in the electric field of the capacitance plus the energy present in the magnetic field of the inductance. When the capacitance is in phase with the magnetic field, both are measured to peak at the same time. This "resistive" condition is found in a transmission line when there are no standing waves. Under resistive conditions, the electric field and inductive field merge into one electromagnetic field that carries only one energy. The identical charges carry both electric and magnetic fields, with the fields in a ratio defined as impedance. Each field is a separate way of looking at the same energy. So from your expressions above U = (CV^2)/2 + (LI^2)/2 You may have been reading about traveling waves. They offer an explaination for how magnetic and electric fields may get out of phase. When the two fields are out of phase, the U = (CV^2)/2 + (LI^2)/2 calculation will ALWAYS sum to more energy than can be found in the resistive wave. This occurs because more energy actually is resident on the line with reflections, due to waves traveling in two directions. The reflection effectively doubles the length of the transmission line available for energy storage. If P = (v^2)/r = (i^2)r is correct, what is the precondition that MUST be true? Answer: The i and v measurements must be across a pure resistance, without reactance. This is why it is often better just to use the original equation: P(t) = V(t) * I(t) for it is always true and requires no preconditions. I learned long ago that it DOES have a precondition. The power measured will only be resistive if measured across a pure resistance. If the measurement is across resistance plus reactance, then reactive power is also measured so P(t) = V(t) * I(t) becomes the sum of an unknown mix of two or more waves. The traveling wave is considered to have a pure resistive impedance. This going by measurements makes things hard! *Too bad we can't see and feel the wave with our own eyes and hands! At a disconinuity, we find a doubling of the voltages, not an increase of 1.414. *This leads me to believe that the crossing pulses never stop in a physical sense. *They do stop in the sense that power is not delived through the center point. ...Keith 73, Roger, W7WKB- Hide quoted text - ...Keith 73, Roger, W7WKB |
Standing-Wave Current vs Traveling-Wave Current
On Jan 11, 10:06*pm, Richard Clark wrote:
On Fri, 11 Jan 2008 18:51:07 -0800 (PST), Keith Dysart wrote: If you cannot identify the source, then you cannot proclaim a separation. That is hardly difficult. If no energy every crosses the middle of the line, Hi Keith, If indeed. * The difficulty is *you've already allowed that the energy is not tagged, so its source is unknown at the load. *So "if" fails through this immutable correlation. *The separation is not demonstrated. Take two flashlights. I claim that the energy for the light produced by each originates in the battery in each flashlight. Is your claim otherwise? Connect the negative terminals of the batteries together. I claim that the energy for the light produced by each still originates in the battery in each flashlight. Is your claim otherwise? Connect the positive terminals of the batteries together through an ammeter. For the purposes of this experiment, the batteries have exactly the same voltage so the ammeter indicates that no current ever flows between the batteries. I claim that the energy for the light produced by each still originates in the battery in each flashlight. Is your claim otherwise? ...Keith |
Standing-Wave Current vs Traveling-Wave Current
GO GUYS GO!
over 700 messages in this thread now, it would probalby be over 1000 already if it hadn't had some contributions sucked away by the 'standing morphing power ranger waves and other stupid stuff' thread! |
Standing-Wave Current vs Traveling-Wave Current
On Jan 12, 2:08*am, Roger Sparks wrote:
On Fri, 11 Jan 2008 18:49:20 -0800 (PST) Keith Dysart wrote: On Jan 11, 7:30*pm, Roger Sparks wrote: On Fri, 11 Jan 2008 13:59:47 -0800 (PST) Keith Dysart wrote: On Jan 11, 11:15*am, Roger Sparks wrote: On Thu, 10 Jan 2008 18:52:28 -0800 (PST)Keith Dysart wrote: P(t) = V(t) * I(t) by substitution from V = I * R P(t) = V(t) * V(t) / R and P(t) = I(t) * I(t) * R Correct. But recall that power is the flow of energy per unit time. The energy present in any section of line is the energy present in the electric field of the capacitance plus the energy present in the magnetic field of the inductance. When the capacitance is in phase with the magnetic field, both are measured to peak at the same time. *This "resistive" condition is found in a transmission line when there are no standing waves. *Under resistive conditions, the electric field and inductive field merge into one electromagnetic field that carries only one energy. *The identical charges carry both electric and magnetic fields, with the fields in a ratio defined as impedance. Each field is a separate way of looking at the same energy. I am not quite sure what you are attempting to say here and whether you are disagreeing with my assertion that the total energy in a section of line is equal to the sum of the energy present in the capacitance and the energy present in the inductance. So from your expressions above U = (CV^2)/2 + (LI^2)/2 You may have been reading about traveling waves. *They offer an explaination for how magnetic and electric fields may get out of phase. *When the two fields are out of phase, the U = (CV^2)/2 + (LI^2)/2 calculation will ALWAYS sum to more energy than can be found in the resistive wave. *This occurs because more energy actually is resident on the line with reflections, due to waves traveling in two directions. *The reflection effectively doubles the length of the transmission line available for energy storage. * This seems like a complicated way to think about things. So complicated that I will not comment on correctness. If P = (v^2)/r = (i^2)r is correct, what is the precondition that MUST be true? Answer: The i and v measurements must be across a pure resistance, without reactance. This is why it is often better just to use the original equation: P(t) = V(t) * I(t) for it is always true and requires no preconditions. I learned long ago that it DOES have a precondition. *The power measured will only be resistive if measured across a pure resistance. *If the measurement is across resistance plus reactance, then reactive power is also measured so P(t) = V(t) * I(t) becomes the sum of an unknown mix of two or more waves. * * This too seems like a complicated way to think about things. P(t) = V(t) * I(t) is simple, and always holds. One does not need to consider the wave content in any way. Or impedances. Measure the instaneous voltage and the instanteous current; multiplying will always yield the instantaneous power. Integrating instantaneous power will always yield the net energy transfer over the interval of integration. ...Keith |
Standing-Wave Current vs Traveling-Wave Current
On Jan 12, 2:08 am, Roger Sparks wrote:
I learned long ago that it DOES have a precondition. The power measured will only be resistive if measured across a pure resistance. If the measurement is across resistance plus reactance, then reactive power is also measured so P(t) = V(t) * I(t) becomes the sum of an unknown mix of two or more waves. In power engineering, the power can consist of two components, active power, V*I*cos(A) = watts, and reactive power, V*I*sin(A) = VARS. These terms are defined in The IEEE Dictionary. P=V*I results in Volt*Amperes, part active and part reactive if the voltage and current are not in phase. -- 73, Cecil, w5dxp.com |
Standing-Wave Current vs Traveling-Wave Current
On Jan 12, 8:10 am, Keith Dysart wrote:
P(t) = V(t) * I(t) is simple, and always holds. But one must remember the units of that result is Volt*Amps, not watts. -- 73, Cecil, w5dxp.com |
Standing-Wave Current vs Traveling-Wave Current
On Sat, 12 Jan 2008 03:49:18 -0800 (PST), Keith Dysart
wrote: Take two flashlights. I claim that the energy for the light produced by each originates in the battery in each flashlight. Is your claim otherwise? Connect the negative terminals of the batteries together. I claim that the energy for the light produced by each still originates in the battery in each flashlight. Is your claim otherwise? Connect the positive terminals of the batteries together through an ammeter. For the purposes of this experiment, the batteries have exactly the same voltage so the ammeter indicates that no current ever flows between the batteries. I claim that the energy for the light produced by each still originates in the battery in each flashlight. Is your claim otherwise? Hi Keith, You have admitted that energy dissipated in the loads cannot be identified to its source and you have used the above devices previous to that statement. Your admission dismisses their applicability. Separability is not demonstrated. 73's Richard Clark, KB7QHC |
Standing-Wave Current vs Traveling-Wave Current
On Sat, 12 Jan 2008 12:32:35 GMT, "Dave" wrote:
over 700 messages in this thread now, it would probalby be over 1000 already if it hadn't had some contributions sucked away by the 'standing morphing Chip, This is not a terribly different posting from your own complaint. 73's Richard Clark, KB7QHC |
Standing-Wave Current vs Traveling-Wave Current
On Jan 12, 11:13*am, Cecil Moore wrote:
On Jan 12, 8:10 am, Keith Dysart wrote: P(t) = V(t) * I(t) is simple, and always holds. But one must remember the units of that result is Volt*Amps, not watts. You really should put a bit of effort into understanding the different expressions for power. P(t) = V(t) * I(t) is saying that the function which describes power with respect to time, P(t), is the product of the function describing voltage with respect to time, V(t), and the function describing current with respect to time, I(t). As corollary, the power at an instant of time is equal to the voltage at that instant times the current at that instant. And, of course the unit watts is the same as the units volts times amperes. Just do the substitution. V = J/C A = C/s V A = (J/C) x (C/s) = J/s = W You are confused with the common use in power engineering where VA is used to mean Vrms*Irms. Whether VA is equal to watts depends on the phase relationship of the voltage and current. When the voltage and current are not in phase, then the expression Pavg = Vrms * Irms * cos(A) can be used to derive the average power. This is a special case of P(t) = V(t) * I(t). It is applicable when V(t) is a sinusoid of a single frequency, and I(t) is related to V(t) using the expression V(t) = Z * I(t). Pavg = Vrms * Irms * cos(A) is completely derived from P(t) = V(t) * I(t) by appropriately substituting for V(t) and I(t) and then averaging P(t) over an appropriate interval (typically one cycle). Bottom line: P(t) = V(t) * I(t) is always correct. The other variations only work when applied under the appropriate conditions. ...Keith |
Standing-Wave Current vs Traveling-Wave Current
On Jan 12, 1:22 pm, Keith Dysart wrote:
P(t) = V(t) * I(t) As corollary, the power at an instant of time is equal to the voltage at that instant times the current at that instant. You obviously mean the *real* instantaneous voltage times the *real* instantaneous current. You should say that to avoid confusion. Seems you need to add 'Re' to that equation to remove the obvious ambiguity. P(t) = Re[V(t)]*Re[I(t)] From "Fields and Waves", by Ramo & Whinnery: W(t) = {Re[Vm*e^j(wt+A1)]}{Re[Im*e^j(wt+A2)]} -- 73, Cecil, w5dxp.com |
Standing-Wave Current vs Traveling-Wave Current
On Jan 12, 2:05*pm, Cecil Moore wrote:
On Jan 12, 1:22 pm, Keith Dysart wrote: P(t) = V(t) * I(t) As corollary, the power at an instant of time is equal to the voltage at that instant times the current at that instant. You obviously mean the *real* instantaneous voltage times the *real* instantaneous current. You should say that to avoid confusion. Seems you need to add 'Re' to that equation to remove the obvious ambiguity. P(t) = Re[V(t)]*Re[I(t)] From "Fields and Waves", by Ramo & Whinnery: W(t) = {Re[Vm*e^j(wt+A1)]}{Re[Im*e^j(wt+A2)]} -- 73, Cecil, w5dxp.com Good recovery. But, of course, V(t) and I(t) are general functions of time. In particular, the discusion was regarding pulses. Only when one constrains oneself to sinusoids and chooses to use the complex exponential notation is it necessary to use Re[]. But it was a good recovery. ...Keith |
Standing-Wave Current vs Traveling-Wave Current
On Jan 12, 3:25 pm, Keith Dysart wrote:
Only when one constrains oneself to sinusoids and chooses to use the complex exponential notation is it necessary to use Re[]. I think that's a false statement. Do you have any proof? Why would the imaginary part of a pulse produce any power? -- 73, Cecil, w5dxp.com |
Standing-Wave Current vs Traveling-Wave Current
On Jan 12, 3:25 pm, Keith Dysart wrote:
But, of course, V(t) and I(t) are general functions of time. In particular, the discusion was regarding pulses. Pulses can be analyzed as Fourier sinusoidal functions with multiple frequencies. Point is that you could have saved a month of grief on this newsgroup if you had initially said your power equation applied only to real voltage and real current. If you had done that, nobody would have argued with you. -- 73, Cecil, w5dxp.com |
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