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#1
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"Richard Clark" wrote - "It was the best of times, it was the worst of times." ============================= Richard, now you're plagiarising Charles Dickens. ---- Reg. |
#2
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"Reg Edwards" wrote in message ... "Richard Clark" wrote - "It was the best of times, it was the worst of times." ============================= Richard, now you're plagiarising Charles Dickens. ---- Reg. Cecil, define 'sloshing.' Walt,W2DU |
#3
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Walter Maxwell wrote:
Cecil, define 'sloshing.' Hi Walt, I'm having trouble with my news-server so I am posting from Google using procedures to which I am not accustomed. The classic wave reflection model indicates that forward power travels from the source to the load where it is incident upon the load. At a load mismatch, some of the forward power is rejected and travels back from the load toward the source as a reflected wave. For instance, in the following lossless example, we have 104.17 watts of forward wave and 4.17 watts of reflected wave on the 75 ohm line. This is all in line with "Reflections" and my unpublished article. 100W--50 ohm line--+--1/4WL 75 ohm line---112.5 ohm load As I infer/understand what Roy, and others, have said while objecting to the material in my unpublished article: The only real forward power wave is the one that is dissipated in the load. The reflected power wave doesn't travel from the load back toward the source and the extra 4.17 watts in the forward wave doesn't travel from the match point back toward the load. The energy associated with the reflected waves just "sloshes" around in the transmission line and doesn't move very far or very fast and certainly not in the form of EM wave components. So Roy's use of the word "slosh" in the context in which he used it, is all I can give you. Roy hasn't defined the word and neither has the IEEE. :-) -- 73, Cecil http://www.qsl.net/w5dxp |
#4
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Cecil, W5DXP, quoting others, wrote:
"The reflected power wave doesn`t travel from the load back toward the source and the extra 4.17 watts in the forward wave doesn`t travel from the match point back toward the load." Users of the Bird and Similar wattmeters know that is what they see. Source and load power is the forward power minus the reflercted power. Zo of the coax enforces its volt to amp ratio on both the incident and reflected waves. Reflected power is again reflected at the match point because the matched source sees no reflection. That`s the point of producing a match in the load. Best regards, Richard Harrison, KB5WZI |
#5
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Richard Harrison wrote:
Users of the Bird and Similar wattmeters know that is what they see. Source and load power is the forward power minus the reflercted power. But that's only what is printed on the meter scale. It doesn't make the "reflected power" real. For the (n+1)th time: the Bird so-called "wattmeter" does NOT sense forward and reflected power. It only senses RF voltage and current on the line. The meter scale calibration is a mathematical operation that depends on a lot of assumptions... most notably the assumption that "reflected power" has some physical reality. I am genuinely open-minded about that debate - which makes the all the more determined to be ruthless about bogus arguments on either side. And the most bogus argument of all is: "Users of the Bird and Similar wattmeters know that is what they see." -- 73 from Ian GM3SEK 'In Practice' columnist for RadCom (RSGB) http://www.ifwtech.co.uk/g3sek |
#6
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Ian White GM3SEK wrote:
But that's only what is printed on the meter scale. It doesn't make the "reflected power" real. I am genuinely open-minded about that debate - which makes the all the more determined to be ruthless about bogus arguments on either side. Ian, correct me if I'm wrong, but I infer that you are biased toward the "no reflected energy waves" side. That bias could be based on perceived knowledge. Seems to me, some people are begging the question. They assume there is no energy in reflected waves and call what the other side says, "gobbleygook", even when presented in scientific terms. I think we all understand the concepts behind net energy. What is in dispute is the next lower layer of dynamic energy movement in both directions at the same time during steady-state. So would you explain what happens to the reflections of a laser beam when aimed at a perfect mirror in free space. Offset the laser beam slightly from normal incidence to start with and observe the reflections with your naked eye. Then bring the beam to 90 degree incidence with the mirror. You can no longer see the reflections but now you can detect the superposition of the forward and reflected waves through interference "rings" or loops with an intensity maximum occuring every half wavelength and an intensity minimum occuring every half wavelength in between. Where is the EM wave energy just sloshing around and not traveling forward and rearward at the speed of light? -- 73, Cecil http://www.qsl.net/w5dxp ----== Posted via Newsfeeds.Com - Unlimited-Uncensored-Secure Usenet News==---- http://www.newsfeeds.com The #1 Newsgroup Service in the World! 120,000+ Newsgroups ----= East and West-Coast Server Farms - Total Privacy via Encryption =---- |
#7
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Cecil Moore wrote:
But that's only what is printed on the meter scale. It doesn't make the "reflected power" real. I am genuinely open-minded about that debate - which makes the all the more determined to be ruthless about bogus arguments on either side. Ian, correct me if I'm wrong, but I infer that you are biased toward the "no reflected energy waves" side. That bias could be based on perceived knowledge. I am trying very hard not to be biased about the actual problem - but I am very much against your methods of debate. Why should anyone consent to follow you into the realms of optics and laser physics, merely because that's where you want to go? Stand your ground right here on the log, Cecil, and talk strictly and exclusively about RF transmission lines. -- 73 from Ian GM3SEK 'In Practice' columnist for RadCom (RSGB) http://www.ifwtech.co.uk/g3sek |
#8
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Cecil Moore wrote:
So would you explain what happens to the reflections of a laser beam when aimed at a perfect mirror in free space? Offset the laser beam slightly from normal incidence to start with and observe the reflections with your naked eye. Then bring the beam to 90 degree incidence with the mirror. You can no longer see the reflections but now you can detect the superposition of the forward and reflected waves through interference "rings" or loops with an intensity maximum occuring every half wavelength and an intensity minimum occuring every half wavelength in between. Incidentally, there is a very good discussion of standing waves in section 7.1.4 of "Optics", by Hecht, 4th Edition. -- 73, Cecil http://www.qsl.net/w5dxp ----== Posted via Newsfeeds.Com - Unlimited-Uncensored-Secure Usenet News==---- http://www.newsfeeds.com The #1 Newsgroup Service in the World! 120,000+ Newsgroups ----= East and West-Coast Server Farms - Total Privacy via Encryption =---- |
#9
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Richard Harrison wrote: Reflected power is again reflected at the match point because the matched source sees no reflection. I think you put your finger on it, Richard. That's exactly what inspired the 'sloshing energy' comment. 73, ac6xg |
#10
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Jim Kelley wrote:
Richard Harrison wrote: Reflected power is again reflected at the match point because the matched source sees no reflection. I think you put your finger on it, Richard. That's exactly what inspired the 'sloshing energy' comment. Except that the "sloshing energy" comment doesn't have the energy sloshing from the load to the match point and back at the speed of light. As I understand the concept of "sloshing energy" it is sloshing back and forth rather locally between the inductance and the capacitance. -- 73, Cecil http://www.qsl.net/w5dxp |
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