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#1
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Actually, several people (W8JI among them) have measured the output
impedance of common amateur linear amplifiers by at least a couple of methods. The most credible measurements show, interestingly, a value very close to 50 ohms when the amplifier is adjusted for normal operation. [sotto voce] "and yet it moves" - updated to Of course, it doesn't really matter, but people continue to make a big deal out of it. Roy Lewallen, W7EL Hi All, As offered in other postings, I challenged for some to differentiate between themselves as Equipment Operators, Bench Techs, and Cut-And-Paste Theoreticians. The "oomph" we all got from that response was, as I also offered, the uncomfortable groan of avoiding serious testing to instead indulge in eternal debates, the offering of puzzles, and the recitation of dead white men's work. So it follows that I am as responsible as others to differentiate myself to the standards I set - it takes some time, but is not seriously difficult. The quality of that differentiation is clearly in the opprobrium above which maintains "it doesn't really matter" and I can accept that, again, by my own terms of "Does it make more than 1dB difference?" which is more a quantitative test than the philosophical, qualitative assertion that got us here. The difference lies in a particular Engineering Note offered in the 1960's by Hewlett Packard: "Microwave Mismatch Analysis, Application Note 56." This note in turn references the work adopted by the National Bureau of Standards published in IEEE Transactions of Microwave Theory and Techniques, Vol. MTT-11, no. 3, May 1963, p. 179, by R.W. Beatty. These references were then expanded in book form "Microwave Theory and Applications," Stephen F. Adam, Prentice-Hall, 1969. I took my training in the only school of Metrology in the US in 1972 and took these works to heart, by far and away not because they were so much academic (even though they qualify in spades beyond all lesser discussion), but because they were written for real engineers employed in real measure employing real tools. So much for Hubris, my own or others. The simple fact of the matter is that if accuracy is not your cup of tea, you wouldn't have read this far anyway. If you are concerned with accuracy, and by that I mean making valid measurements of RF power, then the Z of your source is exceedingly important in the face of a mismatched load. To wit I offer a simple verification of this observation and the works enumerated above. 1. Take one Ham transmitter capable of supporting 5 to 10W into any load without its ALC engaging and altering the power (this simplifies matters but is not strictly necessary). 2. Obtain four 50 Ohm loads each capable of supporting that same 5 to 10W power without causing any of those loads to change Z (this is NOT as simple as it may seem, but is not that difficult if you don't take it for granted). Power will never be applied for more than 10 seconds in any case during readings (or as long as it takes for your transmitter to settle to a stable power). 3. Obtain a Wattmeter capable of reading both forward and reverse power, where 5W is full scale deflection for the forward and reverse power. 4. You will need an assortment of cables and T connectors (choose your own connector style suitable for the frequency that you can support these methods to be described, following). 5. Confirm ALL loads do not exhibit a reverse power reading for full power (that same 5 to 10W) applied to them, one at a time, through each and every cable. 5a. For the purposes of my demonstration, I employed a device of my own design that I call my BVT, a Binary Variable Transmission line. It contains an assortment of coaxial lines arranged such that they can be inserted, inline, in 1 foot increments, for 0 through 32 feet. If this sounds familiar, it was the subject of my very first posting to this group some 8 years ago. 6. Apply one of those 50 Ohm loads in parallel, directly across the transmitter output. Use a T connector to allow another line to be connected in parallel as well. This port will be called the "Plane of the Source." 7. Combine the remaining (3) 50 Ohm loads in parallel using two T connectors such that one port remains open to accept a line to be connected in parallel as well. This port will be called the "Plane of the Load." 8. Connect a length of transmission line from the Plane of the Source to the input of the Power Meter; and in turn, connect another line from the output of the Power Meter to the Plane of the Load. The center of the Power Meter (actually one port or the other depending on which line you will vary in the future) is the "Plane of the Measurement." 8a. I have chosen to use a 2 foot line to the input of the Power Meter; and at the output of the power meter I have a 3 foot line connecting to the BVT (which contains 1 foot of line in the zero position) with another 3 foot line at the BVT output to the Plane of the Load. As such, I had the capacity to change the position of the Plane of the Measurement by 32 feet by one foot additions from a minimum separation of roughly 8 feet. This also elongates the distance between the Planes of the Source and Load from 8 feet to a maximum of 40 feet. 9. I selected 24.9MHz by accident of meeting the Power Meter's sensitivity and the transmitter's capacity to load this enormous mismatch - it also happened to be eminently suitable for the data that follows. ALL data was taken by first setting the output power to force a forward power reading of 5W (full scale) for EVERY variation, and then taking the reverse power reading: Initial reading 1.70W reverse added 1 foot 1.45W 2 1.20W 3 0.95W 4 0.80W 5 0.60W 6 0.50W 7 0.45W 8 0.75W 9 0.80W 10 0.90W 11 1.00W 12 1.20W 13 1.30W 14 1.40W 15 1.45W So, by now it may become apparent that: there is only one mismatched system condition; that condition is not impacted by any ALC action (either through it not being engaged, or being nullified by maintaining a constant forward power); no change in the line conditions inject any additional mismatch (the BVT is flat through all settings 0-15); there is a substantial difference in what the apparent Power is. there is a substantial difference in what the apparent SWR is. The power determination for this system mismatched condition, i.e. a power meter between two Planes of discontinuity, exhibits a low of 3.30W to a high of 4.55W depending on its position in, and the length of the path between the Planes of discontinuity. Hence the answer to the question of what difference does it make? -1.395dB Which also answers my standard: does it make more than 1dB difference? Yes It then follows that for a source that exhibits a 1:2 mismatch that is feeding a 1:3 mismatch through a 50 Ohm system, you can always expect some error, and that if you are ignorant of the dimensions, that error can be as great as roughly 1.4dB. What do the experts calculate? Well, I won't go into that math, that is left to the student to find through research from any of the three references cited. The graphs offered by each of them only allow for a 2:1 mismatched source facing a 2:1 mismatched load which in turn will yield up to a 1dB error. Why the deliberated mismatch at the source? It refutes the myopic discussion of source Z by rendering a known value in parallel with an unknown (sic) which, when is 50 Ohms in itself, must render a source that is NOT 50 Ohms (guaranteed in fact, and supported by the evidence of data forecast by methods adopted by NBS). 73's Richard Clark, KB7QHC |
#2
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who started this topic anyway????
I give up! BUm p.s. match 'em, don't worry about redeflections what a piece d'resistance or d'impedance? |
#3
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ZZZZZZZZZINGGGGG------
(My Head) Guess I am still at the lowly 'operator' stage. ![]() "Richard Clark" wrote in message ... Actually, several people (W8JI among them) have measured the output impedance of common amateur linear amplifiers by at least a couple of methods. The most credible measurements show, interestingly, a value very close to 50 ohms when the amplifier is adjusted for normal operation. [sotto voce] "and yet it moves" - updated to Of course, it doesn't really matter, but people continue to make a big deal out of it. Roy Lewallen, W7EL Hi All, As offered in other postings, I challenged for some to differentiate between themselves as Equipment Operators, Bench Techs, and Cut-And-Paste Theoreticians. The "oomph" we all got from that response was, as I also offered, the uncomfortable groan of avoiding serious testing to instead indulge in eternal debates, the offering of puzzles, and the recitation of dead white men's work. So it follows that I am as responsible as others to differentiate myself to the standards I set - it takes some time, but is not seriously difficult. The quality of that differentiation is clearly in the opprobrium above which maintains "it doesn't really matter" and I can accept that, again, by my own terms of "Does it make more than 1dB difference?" which is more a quantitative test than the philosophical, qualitative assertion that got us here. The difference lies in a particular Engineering Note offered in the 1960's by Hewlett Packard: "Microwave Mismatch Analysis, Application Note 56." This note in turn references the work adopted by the National Bureau of Standards published in IEEE Transactions of Microwave Theory and Techniques, Vol. MTT-11, no. 3, May 1963, p. 179, by R.W. Beatty. These references were then expanded in book form "Microwave Theory and Applications," Stephen F. Adam, Prentice-Hall, 1969. I took my training in the only school of Metrology in the US in 1972 and took these works to heart, by far and away not because they were so much academic (even though they qualify in spades beyond all lesser discussion), but because they were written for real engineers employed in real measure employing real tools. So much for Hubris, my own or others. The simple fact of the matter is that if accuracy is not your cup of tea, you wouldn't have read this far anyway. If you are concerned with accuracy, and by that I mean making valid measurements of RF power, then the Z of your source is exceedingly important in the face of a mismatched load. To wit I offer a simple verification of this observation and the works enumerated above. 1. Take one Ham transmitter capable of supporting 5 to 10W into any load without its ALC engaging and altering the power (this simplifies matters but is not strictly necessary). 2. Obtain four 50 Ohm loads each capable of supporting that same 5 to 10W power without causing any of those loads to change Z (this is NOT as simple as it may seem, but is not that difficult if you don't take it for granted). Power will never be applied for more than 10 seconds in any case during readings (or as long as it takes for your transmitter to settle to a stable power). 3. Obtain a Wattmeter capable of reading both forward and reverse power, where 5W is full scale deflection for the forward and reverse power. 4. You will need an assortment of cables and T connectors (choose your own connector style suitable for the frequency that you can support these methods to be described, following). 5. Confirm ALL loads do not exhibit a reverse power reading for full power (that same 5 to 10W) applied to them, one at a time, through each and every cable. 5a. For the purposes of my demonstration, I employed a device of my own design that I call my BVT, a Binary Variable Transmission line. It contains an assortment of coaxial lines arranged such that they can be inserted, inline, in 1 foot increments, for 0 through 32 feet. If this sounds familiar, it was the subject of my very first posting to this group some 8 years ago. 6. Apply one of those 50 Ohm loads in parallel, directly across the transmitter output. Use a T connector to allow another line to be connected in parallel as well. This port will be called the "Plane of the Source." 7. Combine the remaining (3) 50 Ohm loads in parallel using two T connectors such that one port remains open to accept a line to be connected in parallel as well. This port will be called the "Plane of the Load." 8. Connect a length of transmission line from the Plane of the Source to the input of the Power Meter; and in turn, connect another line from the output of the Power Meter to the Plane of the Load. The center of the Power Meter (actually one port or the other depending on which line you will vary in the future) is the "Plane of the Measurement." 8a. I have chosen to use a 2 foot line to the input of the Power Meter; and at the output of the power meter I have a 3 foot line connecting to the BVT (which contains 1 foot of line in the zero position) with another 3 foot line at the BVT output to the Plane of the Load. As such, I had the capacity to change the position of the Plane of the Measurement by 32 feet by one foot additions from a minimum separation of roughly 8 feet. This also elongates the distance between the Planes of the Source and Load from 8 feet to a maximum of 40 feet. 9. I selected 24.9MHz by accident of meeting the Power Meter's sensitivity and the transmitter's capacity to load this enormous mismatch - it also happened to be eminently suitable for the data that follows. ALL data was taken by first setting the output power to force a forward power reading of 5W (full scale) for EVERY variation, and then taking the reverse power reading: Initial reading 1.70W reverse added 1 foot 1.45W 2 1.20W 3 0.95W 4 0.80W 5 0.60W 6 0.50W 7 0.45W 8 0.75W 9 0.80W 10 0.90W 11 1.00W 12 1.20W 13 1.30W 14 1.40W 15 1.45W So, by now it may become apparent that: there is only one mismatched system condition; that condition is not impacted by any ALC action (either through it not being engaged, or being nullified by maintaining a constant forward power); no change in the line conditions inject any additional mismatch (the BVT is flat through all settings 0-15); there is a substantial difference in what the apparent Power is. there is a substantial difference in what the apparent SWR is. The power determination for this system mismatched condition, i.e. a power meter between two Planes of discontinuity, exhibits a low of 3.30W to a high of 4.55W depending on its position in, and the length of the path between the Planes of discontinuity. Hence the answer to the question of what difference does it make? -1.395dB Which also answers my standard: does it make more than 1dB difference? Yes It then follows that for a source that exhibits a 1:2 mismatch that is feeding a 1:3 mismatch through a 50 Ohm system, you can always expect some error, and that if you are ignorant of the dimensions, that error can be as great as roughly 1.4dB. What do the experts calculate? Well, I won't go into that math, that is left to the student to find through research from any of the three references cited. The graphs offered by each of them only allow for a 2:1 mismatched source facing a 2:1 mismatched load which in turn will yield up to a 1dB error. Why the deliberated mismatch at the source? It refutes the myopic discussion of source Z by rendering a known value in parallel with an unknown (sic) which, when is 50 Ohms in itself, must render a source that is NOT 50 Ohms (guaranteed in fact, and supported by the evidence of data forecast by methods adopted by NBS). 73's Richard Clark, KB7QHC |
#4
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On Sun, 20 Jul 2003 23:38:47 -0500, "WavyDave"
wrote: ZZZZZZZZZINGGGGG------ (My Head) Guess I am still at the lowly 'operator' stage. ![]() Lowly only if you have any pretensions about being expert in the field of power measurement - and come to some other conclusion that is indefensible. If not, enjoy the hobby for what you seek in it. Even equipment operators can put these issues to good use (or bad use in the sense that follows) if you participate in a Shoot-Out and use an amplifier with other than 50 Ohm output Z feeding an antenna with other than 50 Ohm input Z. Through hi-grading the 50 Ohm feedline to select that choice position along it for the Judges' Wattmeter, you can shave yourself 1 or 2dB advantage over the others through their ignorance of the Mismatch Error. Of course, this is almost certainly a common condition and everyone is in the dark. So are the results, but what the hey, its only a game. I offer the cutting line at "does it make more than 1dB difference" to offer a qualitative assessment. Personally, and as a belief, I rarely care about 3 or 6dB (more or less); hence 1dB is extremely liberal in their favor (and they rarely even meet that gracious low-ball). It is only the cut-and-paste theoreticians that demand their solutions are more accurate than nature can guarantee - and that it does make a difference. Such is the stuff of CFA and EH claims. 73's Richard Clark, KB7QHC |
#5
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On Sun, 20 Jul 2003 10:50:35 -0000, "David Robbins"
wrote: Actually, several people (W8JI among them) have measured the output impedance of common amateur linear amplifiers by at least a couple of methods. The most credible measurements show, interestingly, a value very close to 50 ohms when the amplifier is adjusted for normal operation. but is that a real resistive 50 ohms, or a dissipationless 50 ohms non-resistive? or could it be a virtual 50 ohms hiding some other fake steady state value? What would make it real for you? you can't read it when you connect an ohm meter to the output connector, so how can it be a resistance? You can't read a 50 Ohm resistor with an Ohmmeter through a 0.1 µF capacitor either, would you hold one while you pour a KW at 10M to the series pair? or is it really a complex impedance that can be ignored when you calculate the output power? I used real loads. I can repeat this with reactive ones, but it will only shift the curve of data. but then again it might be due to internal reflections making it an infinite sum of many other factors? That is the entire point and expressly demonstrated between the mismatched plane of the source and the mismatched plane of the load. maybe we have to learn how to conjugate our impedances before we can have a decent discussion about it? Care to give an example? but what if its only a matching system to free space impedance? when there are reflections does it reflect or absorb? who started this topic anyway???? Hi David, What if? What is reflecting? In this case BOTH the source AND the load. If you wish, we can jimmy up the load to present 377 Ohms and drive the error of power determination even higher (probably on the order of 50-80%). However, to this point two hours of work is sufficient to demonstrate this if anyone wishes to confirm my analysis. To this point a couple of days has revealed no data to have refuted my analysis. Denial is an option and opinion is free. Even at this steep discount none step up to the bench. I didn't expect anyone would anyway. ;-) 73's Richard Clark, KB7QHC |
#6
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On Sun, 20 Jul 2003 08:05:05 -0700, W7TI wrote:
On Sun, 20 Jul 2003 07:21:07 GMT, Richard Clark wrote: The "oomph" we all got from that response was, as I also offered, the uncomfortable groan of avoiding serious testing to instead indulge in eternal debates, the offering of puzzles, and the recitation of dead white men's work. _________________________________________________ ________ And while you're doing all that testing and measuring, I will have Worked All Stations. :-) -- 73, Bill W7TI Hi Bill, You cover a lot of ground in 2 hours then. QSL cards must be pasted to your walls 6 inches deep, ceiling to floor. Even at a quarter inch deep you qualify well beyond the "oomph" spectacularly demonstrated by others. ;-) 73's Richard Clark, KB7QHC |
#7
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Richard Clark wrote:
To this point a couple of days has revealed no data to have refuted my analysis. Denial is an option and opinion is free. Even at this steep discount none step up to the bench. I didn't expect anyone would anyway. ;-) Please state your conclusions in concepts that people can understand. -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 80,000 Newsgroups - 16 Different Servers! =----- |
#8
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On Tue, 22 Jul 2003 05:10:00 -0500, W5DXP
wrote: Richard Clark wrote: To this point a couple of days has revealed no data to have refuted my analysis. Denial is an option and opinion is free. Even at this steep discount none step up to the bench. I didn't expect anyone would anyway. ;-) Please state your conclusions in concepts that people can understand. Hi Cecil, This was not a monograph for the Sunday Supplement. Those who understand the concepts of reflection are aware of the implications. Feel free to abandon the topic if you find the report too difficult to follow as I am not offering any amendments nor advancing any speculations. Debate is not a goal here. If, on the other hand you have new data to offer; please feel free to post it. 73's Richard Clark, KB7QHC |
#9
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Richard Clark wrote:
wrote: Please state your conclusions in concepts that people can understand. Those who understand the concepts of reflection are aware of the implications. Feel free to abandon the topic if you find the report too difficult to follow as I am not offering any amendments nor advancing any speculations. Can we assume that you are incapable of stating your conclusions in concepts that people can understand? In other words, what was the purpose of your posting? -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 80,000 Newsgroups - 16 Different Servers! =----- |
#10
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David J. Windisch wrote:
I quote, in part, from my original post: "State"? Do you mean "write" or "post"? "state - to set forth formally in speech or writing" "conclusions"? DYM "opinions"? With references, a/o bibliography?: "conclusion - a result, issue, or outcome" "concepts"? What DYM ? New or old? "concept - an idea of something formed by mentally combining all its characterstics" Sorry David, I had no idea in the world what "DYM" means. So how the heck can you get aggravated at me for my ignorance of "DYM"? Do you know what "SCADA" means? Am I allowed to get angry at you if you don't know? -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 80,000 Newsgroups - 16 Different Servers! =----- |