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#41
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Roy wrote -
If you have some other "rho" you want to argue about, please call it something else. =========================== - - - and while you are about it change the name of the SWR meter. |
#42
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On Wed, 03 Sep 2003 18:50:08 -0500, Cecil Moore
wrote: Since you snipped my posting, I have no idea what it was all about. Hi Cecil, I didn't this time, and I doubt you are any further ahead. Perhaps you suffer from the Motorola syndrome of confusion. ;-) So, is your response to the offer of the bridge description Yes? or No? (Consult google to fill the short attention span problems.) 73's Richard Clark, KB7QHC |
#43
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So, do you want the bridge description or not?
Richard Clark, KB7QHC ============================ Rich, pleased to receive a message from you succinct enough to read. ;o) But it looks like there's at least two contestants who have now vanished from the thread. Keep stirring it up. |
#44
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On Thu, 4 Sep 2003 00:38:54 +0000 (UTC), "Reg Edwards"
wrote: So, do you want the bridge description or not? Richard Clark, KB7QHC ============================ Rich, pleased to receive a message from you succinct enough to read. ;o) But it looks like there's at least two contestants who have now vanished from the thread. Keep stirring it up. How do you mix an ingredient of one? That query alone will bring in at least a dozen recipes. ;-) |
#45
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Cecil Moore wrote:
wrote: And yes, |rho| can be greater than unity for a passive load. But the power reflection coefficient cannot be greater than 1.0 which is what the argument is all about. Which is entirely consistent with my previous statement: It follows that when rho is greater than unity, it is not 'physically meaningful to separate the total power as the sum of the incident and reflected power' so the equation |rho| = Sqrt(Pref/Pfwd) has no meaning. I suppose one might phrase it as 'there is no such thing as a power reflection coefficient' when it is not 'physically meaningful to separate the total power as the sum of the incident and reflected power'. ....Keith |
#46
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Cecil Moore wrote:
Reg Edwards wrote: Roy wrote - If you have some other "rho" you want to argue about, please call it something else. - - - and while you are about it change the name of the SWR meter. Trouble is, (Z2-Z1)/(Z2+Z1) is not always equal to Sqrt(Pref/Pfwd) What then? The equality was always iffy when you don't take the absolute value. But once you do, the equality may hold depending on the equations you use to derive Pref and Pfwd. Whether Pref or Pfwd represent something physically meaningful is another question, also dependent on how you derive them. ....Keith |
#47
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Keith wrote:
"I suppose one might phrase it as "There is no such thing as a power reflection coefficient" when it is not physically meaningful to separate the total power as the sum of the incident and reflected power so the equatiomn: [rho] = sq. rt. (Pref / Pfwd) has no meaning." We don`t have a choice of options on a menu to select or reject from. Reality is whatever it is and we accept it and describe it as best we can. Terman says on page 97 of his 1955 edition: "{rho} = (SWR-1) / SWR + 1." Power varies as the equare of the voltage, because when you increase the volts you also automatically increase the amps (Ohm`s law). Thus, Terman has a subscript at the bottom of page 97 which is relevant: "The definition of standing-wave ratio is sometimes called voltage standing-wave ratio (VSWR) to distinguish it from the standing-wave ratio expressed as a power ratio which is (Emax / Emin) squared." In my long rxperience, I`ve found it`s never profitable to argue with Terman. He is as close to infallible as any wrirter I`ve ever read. Best regards, Richard Harrison, KB5WZI |
#49
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Cecil Moore wrote in message ...
Dr. Slick wrote: And how do you explain the rho 1 for a passive network? Shouldn't be possible. And neither should a negative SWR. This seems to me to be somewhat akin to the fact that s11 and rho can have different values at an impedance discontinuity where a 'third power' is commonplace. Roy's 'third power' at the load appears to be analogous to a re-reflection of some sort as the inductive load tries and fails to dump energy back into the Z0=68-j39 transmission line. A re-reflection is another component of forward power. The ratio of reflected Poynting vector to forward Poynting vector is |rho|^2. In Roy's example, the total average Poynting vector points toward the load indicating that (Pz+ - Pz-) 0. That means |rho|^2 cannot be greater than 1.0. Cecil, The ratio Pref/Pfwd is directly related to the ratio [rho]. Consider that after the absolute value brackets, the phase information is gone. But since we are going to a ratio of average (RMS) values OR peak values of power, it doesn't matter. In other words, if you use V**2/R, the "V" can be either peak or RMS, it doesn't matter, because it is a ratio. And of course, the "R" doesn't matter either. And of course, the phase information is gone with the absolute value brackets. If you agree that the Pref/Pfwd ratio cannot be greater than 1 for a passive network, then neither can the [Vref/Vfwd]= rho be greater than 1 either. Some people wanna rewrite some books here. Slick |
#50
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