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#42
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Tom Donaly wrote:
Here's a more general equation for you Cecil: (A1-A2)*Cos(wt-kx) + 2*A2*Cos(kx+d/2)*Cos(wt+d/2). Yes, it is more general, Tom, but since the subject is standing waves and not traveling waves, it is overly general. Why would you post an equation containing a traveling wave term when the subject is the equation for standing waves? This is the total equation for the condition where power is being delivered to a load in the presence of standing waves. The first term makes it to the load. The second term doesn't. The first term is a traveling wave and indeed does contain phase information. There's no argument about whether a traveling wave contains phase information. The argument is whether the second term, the standing wave term, contains phase information. Gene Fuller says it doesn't, Eugene Hecht says it doesn't, and I'm inclined to agree. -- 73, Cecil http://www.qsl.net/w5dxp |
#43
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wrote:
When you show a track record of being honest and you stop those attacks and your constant distortions of what other people say, I'm sure people will start talking to you again. Of course, you never attack anyone. Pot, Kettle - Kettle, Pot. Here's a smattering of what you have said to me during the past month: W8JI wrote: 3/5/06 "Cecil, You are a horse's ass." 3/10/06 "If you weren't so pig-headed ... Until you stop, put the beer away,..." 3/11/06 "I'm also a victim of Cecil's twicted reality now." 3/11/06 "It would be comical to watch Cecil twist reality if it wasn't sad." 3/11/06 "Cecil's normal tactic is to change what other people say." 3/27/06 "how much will you pay me for putting up with you?" 3/27/06 "I feel sorry for anyone who has to deal with you on a daily basis. No wonder your wife split." -- 73, Cecil http://www.qsl.net/w5dxp |
#44
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Richard Fry wrote:
But clearly these lengths in degrees do not define the self-resonant length of that radiator. Could it be that the resonant 80 degrees of physical length is 90 degrees of electrical length? -- 73, Cecil http://www.qsl.net/w5dxp |
#45
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wrote in message
ups.com... but we can not use electrical degrees to 'splain the behavior of coiled antenna wire? I can see how problems could arise going by the length of coil wire length in degrees only. Lets say you run a coil 1 foot from the base. Lets say that coil uses 25 turns to tune a particular frequency. Now, move the coil up 2 ft higher, and see if that same 25 turns will tune the same frequency. It won't. You will have to add a few more turns. So just going by the total mast plus coil wire length in degrees could vary all over the map just by changing the position of the coil. As you raise the coil, you will have to add more and more of "degrees" of wire to tune the same frequency. :/ Dunno...There may well be some variation of current from the bottom vs the top of the coil, but overall, I still view the operation of a loading coil as a "lumped" mechanism overall. Even if you all decide that the current changes, or it doesn't , it ain't gonna make a hoot's worth of difference in the design of mobile whips. I think it's an argument that has no real value to me as far as mobile whips go. The performance of all the various coil heights, and configs have been well known for years. Coil current taper or not. I just don't see the facination with arguing about something that even if decided one way or the other, still won't make any difference in the final antenna design. Oh well...Continue the tail chasing excercise.... I'm outa this one... One post is all I will waste on this subject.. I couldn't mount my coil much higher if I wanted to... Current taper or not. :/ MK MK, that is the whole point, that you portray missing or not appreciating. It might not matter to you if you lose $100, but it might matter to someone else. Same with loading coil. What you are describing, the effect where the coil is located, being known, is the result of the phenomena we are trying to straighten out, explain and apply properly in modeling and design exercises. The position of coil within the antenna has significant effect. The worst is at the base, fewer turns required. The best is somewhere about 2/3 up the radiator, more turns required. You stick it on the top, no stinger or hat, you get it almost invisible. With what we are discussing and defending here is the proper understanding of the current flow in the loading coil and its drop across and its effect on the efficiency of the loaded antenna. Efficiency is proportional to the area under the current curve distribution along the radiator. If you properly model the coil as solenoid or loading stub to see the real drop of current across the coil and its effect in various positions along the radiator, the all is clear and is with agreement with practical experience, antenna shootout results, measurements. As I mentioned numerous times, its effect on design and modeling loaded antenna systems will be even more pronounced, because effect gets magnified when you start adding elements. This is especially important when you try to design super receiving antennas for low bands where F/B and clean pattern is very desirable and is the most critical aspect of antenna design or modeling. It is harder to obtain the max F/B or least rear lobes than to maximize the design for max gain. It might not matter to you, but I am sure many would benefit from knowing more precisely what is REALLY going on and then use or correct their design methodology. I think it is fine for you to ignore this and poh-poh it. But I know how huge difference it made in my 160m mobile antenna when I extended the whip to the front bumper with wire. We are not saying that piece of wire that coil is wound with, has so many electrical degrees. If we carefully consider and understand the phenomena, you would realize that the radiator has same electrical length (say 15 deg) and when you move the coil and ADJUST THE TURNS to bring the antenna back to resonance (90 deg) that coil would "replace, take care of" 75 degrees. The turns have to be adjusted in order to "participate" in the current replacement game. The lesson is, the higher you place the coil on the radiator, the more turns you need to reresonate the radiator, the high current portion of the antenna current distribution curve gets "stretched up", better efficiency (larger area under the overall curve). Then the coil DROPS the current across itself to some lower value, which then continues to drop across the tip and that area, quite smaller adds to the one from the bottom part of the radiator. This all is supported by reality, except "gurus" who insist that the current is (about) the same across the coil and they make (theoretically) antenna current to be higher across the tip and "more" efficient than it is. Again, you stick 6 of those in the 3 el loaded Yagi design and you get GI-GO. It is known how profound effect had replacement of loading stubs by coils in the KLM 3 el. 80 m loaded Yagi. Better gain, huge improvement in the F/B and pattern. Has been done and described. And this is just replacing the same inductance value stub with coil, where delta current from stub wires was enough to throw monkey wrench in the Yagi performance. Now consider larger error from the wrong assumption or calculation caused by wrong current magnitudes and distribution. Again you might not give a hoot about this "trivial" exercise, but if I want to design 4 el loaded quad or Yagi for 80 or 160, it matters a lot. So it just amazes me that some of the smarter heads resist so much in trying to find out reality and develop better consideration of the effect for design and modeling. No technical answers to Cecil's questions and my "from scratch" thread deteriorated into pink electrons and dead end in electrical degrees. So far what we have is the reality, few who are trying to legitimize it and few who got off on the wrong foot, in effort to preserve their (wrong) face they cling to it with scientwific "proofs" why it can't be so, when IT IS. When I tried to go step by technical step through the case, the "gurus" are not there. Cases that Cecil showed in EZNEC model and demonstrating that current across the loading coil (not one in the box) in the antenna can have anything from equal to "nothing" at the other end, depending on its position in the standing wave picture. It all jives with our original argument. We spotted the "problem", we dissected it, thanks to fierce flat earthers, and now have better understanding of the phenomena and can use to design better antennas. I care about antennas, this is the last frontier where we can still improve thing, now with modeling tools. I still operate contests and go for ultimate - beating the all time records, and that's where the edge can be obtained. Heloooo guys! Measure, feel, whatever, the frickin' current across the loading coil and then come back and tell the world why it IS different, but IT CAN'T be so, because you said so in the beginning and you just can't admit being wrong. Reality can't be twisted, just like Earth is not going back to flat! Saying now that is no big deal, not important, will not exonerate the "wrongoes". It is significant not to be ignored. If I was in "their" shoes, I would say: "gee guys, interesting, thanks for bringing it up, explaining it, I guess we were wrong, now we can design better antennas". Stay tuned..... Thanks again Cecil, Richard and others for putting up with and shedding more and more light on the phenomena. It must go down in history as big as Galileo's fight :-) I am glad that, hopefully, nobody will burn us. 73 Yuri, K3BU.us |
#46
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On Tue, 4 Apr 2006 10:32:08 -0400, "Yuri Blanarovich"
wrote: Now consider larger error from the wrong assumption or calculation caused by wrong current magnitudes and distribution. Hi Yuri, Why is it that you can say this so often, and yet never put a number to it? What is the error? You also speak of efficiency. What is the efficiency? Very simple questions. Technically based. Selected because they seem to be of supreme importance to you, and yet you don't seem to have a handle on the situation. 73's Richard Clark, KB7QHC |
#47
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"Cecil Moore" wrote ...
Richard Fry wrote: But clearly these lengths in degrees do not define the self-resonant length of that radiator. Could it be that the resonant 80 degrees of physical length is 90 degrees of electrical length? __________ That a self-resonant, unloaded broadcast radiator length is shorter than the 90 degree conventional "electrical length" defined by the FCC is a given. But this reality sometimes is not recognized. RF |
#48
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Cecil Moore wrote:
John Popelish wrote: Cecil Moore wrote: Compared to zero amps of standing wave current when the forward current phasor and the reflected current phasor are 180 degrees out of phase, just how much effect can capacitance have? A standing wave voltage passes exactly as much (AC RMS) current through a capacitance as a traveling wave voltage does. But the two waves are different as can be seen from their equations. That difference is a difference in the pattern (distribution) of voltage and current along the line, as well as a possible difference in amplitude and phase at any given point. But at any point that is not a node in the standing wave pattern, there will be an ordinary AC voltage or current at some amplitude between double the traveling wave amplitude and zero amplitude, and one of two phases (that switch each time you pass a node). A traveling wave transfers net energy along a transmission line or antenna wire. A standing wave transfers zero net energy along a transmission line or antenna wire. No argument. But a standing wave still represents storage of energy in the line, as with any resonant structure, and that stored energy shows up as magnetic fields and electric fields along the line. The big difference is that the magnetic fields bob up and down at some areas and the electric fields bob up and down half way in between those areas. At any given moment, there is a fixed total energy in the combination of all the magnetic and electric fields. In the areas where the electric field is bobbing up and down, there must be capacitive current caused by that variation in electric field. From "Fields and Waves in Modern Radio", by Ramo & Whinnery, 2nd edition, page 43: "The total energy in any length of line a multiple of a quarterwavelength long is constant, merely interchanging between energy in the electric field of the voltages and energy in the magnetic field of the currents." Exactly. How can you write this, but deny the capacitive current that delivers this electric field energy twice every cycle to all capacitance feeling this voltage swing? Hecht says it best in "Optics" concerning standing waves: "The composite disturbance is then: E = Eo[sin(kx+wt) + sin(kx-wt)] Applying the identity: sin A + sin B = 2 sin 1/2(A+B)*cos 1/2(A-B) yields: E(x,t) = 2*Eo*sin(kx)*cos(wt)" cos(wt) is the AC swing that drives the capacitive current. sin(kx) is the positional variation of that AC voltage along the line. I have absolutely no argument with the expression, only with your understanding of what it says. "This is the equation for a STANDING or STATIONARY WAVE, as opposed to a traveling wave. Its profile does not move through space; it is clearly not of the form Func(x +/- vt)." Profiles do not charge capacitance, instantaneous rate of change of voltage drives current through capacitance. cos(wt) describes a sinusoidal variation of voltage over time (you couldn't have an RMS value of voltage at a point or an RMS value of current past a point, without it. [Standing wave phase] "doesn't rotate at all, and the resultant wave it represents doesn't progress through space - its a standing wave." I suggest you drop talking about phasors, till you understand what cos(wt). Speaking of "... net transfer of energy, for the pure standing wave there is none." But it does represent net storage of energy. The total stored energy is the sum of energies in the two traveling waves over the length. A standing wave does not violate conservation of energy. Storage that must continuously be swapping back and forth from magnetic field energy to electric field energy. When the energy storage is all electric, that implies charges capacitance. Don't give up, the light may be just about to come on. |
#49
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Cecil Moore wrote:
Tom Donaly wrote: Here's a more general equation for you Cecil: (A1-A2)*Cos(wt-kx) + 2*A2*Cos(kx+d/2)*Cos(wt+d/2). Yes, it is more general, Tom, but since the subject is standing waves and not traveling waves, it is overly general. Why would you post an equation containing a traveling wave term when the subject is the equation for standing waves? This is the total equation for the condition where power is being delivered to a load in the presence of standing waves. The first term makes it to the load. The second term doesn't. The first term is a traveling wave and indeed does contain phase information. There's no argument about whether a traveling wave contains phase information. The argument is whether the second term, the standing wave term, contains phase information. Gene Fuller says it doesn't, Eugene Hecht says it doesn't, and I'm inclined to agree. Cecil, I won't try to educate you because it's a waste of time, but for everyone else, consider that in an antenna, there is energy going into, and being radiated out of, the antenna in the form of an electromagnetic wave. Since Cecil says standing waves can't transfer energy from one place to another (he didn't always say this) that means that the only way energy can be radiated is through the traveling wave component of the electromagnetic wave. You would think that this would be important to him in his search for a dumbed down theory of reflection mechanics, but evidently he is more interested in his arguing point concerning Tom R. and Roy measuring current in a standing wave environment than he is in reaching an understanding of what he's talking about. No wonder no one's communicating with him. 73, Tom Donaly, KA6RUH |
#50
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John Popelish wrote:
But at any point that is not a node in the standing wave pattern, there will be an ordinary AC voltage or current at some amplitude between double the traveling wave amplitude and zero amplitude, and one of two phases (that switch each time you pass a node). Please give us the equation for "ordinary AC voltage or current". No argument. But a standing wave still represents storage of energy in the line, as with any resonant structure, and that stored energy shows up as magnetic fields and electric fields along the line. The big difference is that the magnetic fields bob up and down at some areas and the electric fields bob up and down half way in between those areas. At any given moment, there is a fixed total energy in the combination of all the magnetic and electric fields. No argument, and therefore no need for the "But" in your statement. I agree with you but it doesn't change a thing about the real argument. Exactly. How can you write this, but deny the capacitive current that delivers this electric field energy twice every cycle to all capacitance feeling this voltage swing? I don't deny it - never have - never will. Please stop trying to set up straw men. The discussion has *NEVER* be about what happens during one cycle. The current measured by W8JI and W7EL and reported by EZNEC is RMS current. Instantaneous values are just another straw man diversion. Profiles do not charge capacitance, ... I'm glad you agree. Profiles are maximum RMS envelope values and that is what EZNEC reports. [Standing wave phase] "doesn't rotate at all, and the resultant wave it represents doesn't progress through space - its a standing wave." I suggest you drop talking about phasors, till you understand what cos(wt). Hecht and I have been a little lose with words while assuming the readers have a certain knowledge level. For the uninitiated, When Hecht (or I) say the phasor doesn't rotate at all, we mean the phasor doesn't rotate at all with respect to the source phasor. Any initiated person would know that. The phase of the standing waves doesn't change with respect to the phase of the source signal. Hecht assumed you would know what he meant by that statement. Speaking of "... net transfer of energy, for the pure standing wave there is none." A standing wave does not violate conservation of energy. Exactly my point! Nothing violates conservation of energy. If the RMS forward current in the coil is the same magnitude at both ends and the RMS reflected current in the coil is the same at both ends, the conservation of energy principle is satisfied NO MATTER WHAT THE STANDING WAVE CURRENT TURNS OUT TO BE. What is it about that statement that you don't understand? Storage that must continuously be swapping back and forth from magnetic field energy to electric field energy. When the energy storage is all electric, that implies charges capacitance. Again, nobody has ever been discussing what happens within a partial cycle. Discussion of such is obviously a diversionary straw man. Feel free to find someone else willing to discuss it. It is completely irrelevant to this discussion of RMS envelope values. -- 73, Cecil http://www.qsl.net/w5dxp |
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