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#1
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Wow this is a long thread. Don't really know where I should put my two bits
in, but here it goes. I have designed several RF PA sections in the past. 500MHz at about 50W. Pretty easy stuff if you have the right tools and know how to use them. The tools I like using for matching the power output FET is two triple stub tuners. One on the input of the FET and one on the output. So it goes...pre-amp (50 ohm output) - stub tuner - FET - stub tuner - 50 ohm dummy pad - spectrum analyzer. Then just tune the stubs for the performance you desire, these include: efficiency (thermal issues), harmonic content, spurious emissions, load VSWR considerations, cold start, ect. Then remove the FET and look into the triple stub tuners with the network analyzer. Model and duplicate the network out of discrete components that can handle the voltage/power, send the design off to the enviro test lab, and head home early for the day. Cheers, Thomas "gwhite" wrote in message ... Richard Clark wrote: As I've noted in the past, you can fill a library with negative assertions... The troublesome assertion is not the negative one. It is that RF PA's are conjugate matched. Neither you nor Ken has provided a single example of such a design that also extracts the maximum amount of "linear" power from a device and essentially its power supply (after all, that is what it is: a _power_ amp). Your example said nothing about output-Z, which suggests you have no clue, since you didn't even remotely address the issue. For Ken's part, he recently obfuscated by dismissing an example that was primarily intended to be illustrative, but yet holding the salient points. He completely ignored (or didn't understand) the clipping issue. Further obfuscation was provided by talking about "protection circuitry," which may or may not exist in a circuit, but adds zero to a discussion regarding how the PA is to be loaded. "Protection" is a non-stater because the PA is either off or impaired. Ken's argument is circular. He say's that if a design is done for conjugate match, then it will behave as if it is conjugately matched. Well of course (or at least sort of under specific test conditions and circuits)! It is self-fullfilling prophecy but it unfortunately makes no statement regarding obtaining the maximum power out of the circuit in the sense of turning DC power into RF power (yes, *extracting* power from the DC supply and transformed to RF). This is paramount to PA design. To use the device to maximum efficacy, as Cripps puts it, a load-line match is needed. Ken's "conjugate match" design won't do that, and that's why PA's aren't designed that way. The bottom line is that if I design an amp via load line techniques using the same device and power supply as Ken (him using conj-match), my amp will deliver higher unclipped PEP than his. That is the factual result you resist. Now if you want to pay for extra power and big devices, that's your business--go ahead and attempt to conj-match your amp--but engineers who design PA's don't do that. Another idealized and hypothetical example to elucidate the load-line principle is offered. Let's say we have a 10 W FET we'll build into a class A circuit. An RF choke is used to supply drain current. We DC bias it to Vd = 10 V and Id = 1 A. Just for argument sake, let's say it has a constant internal resistance of 110 ohms and the device will break down at 25 V. According to the most idealized and standard load-line theory, we should load it to rL = Vd/Id = 10 Ohms. This idealization includes the definition of positive and negative clipping -- whichever comes "first" -- of being the operational limit for output voltage swing. Clipping is associated with severe distortion. Since we need rL to be 10 ohms, and Ri = 110 ohms, we need to make the actual load resistor equal to: RL = 11 Ohms. Let's check that result and see if it meets the clipping constraint for maximum available power. positive swing = Id*rL = 1*10 = 10 V negative swing = Vd = 10 V Power delivered to RL: Pload = 10^2/(2*11) = 4.55 W The efficiency is a little under 50% because of the internal resistance. Note the Load resistance is decidely not the conjugate of the internal resistance. Let's spot check the load to see if it at least appears to be the peak available power, by testing two loads "immediately" on either side of our optimum 11 ohms. Let RL = 10 ohms positive swing = Id*rL = 1*9.17 = 9.17 V negative swing = Vd = 10 V Since we positive clip at 9.17 V, we are limited by our design clipping constraint to only driving the PA such that 2*9.17 V is the maximum available voltage swing. Power delivered to RL: Pload = 9.17^2/(2*10) = 4.20 W Let RL = 12 ohms positive swing = Id*rL = 1*10.82 = 10.82 V negative swing = Vd = 10 V Since we negative clip at 10 V, we are limited by our design clipping constraint to driving the PA such that 2*10 V is the maximum available voltage swing. Power delivered to RL: Pload = 10^2/(2*12) = 4.17 W Sure enough, the power peaked at a load of 11 ohms, just like load-line theory says it will. Now let's see what the available power hit of conjugate matching is. By definition, conj-match insists RL = Ri = 110 ohms. Again we are limited in our clipping constraint by static drain current, and supply voltage, specifically 10 V. Our negative swing limit is, as ever, 10 V (the drain voltage). positive swing = Id*rL = 1*55 = 55 V This would breakdown the device, but the lower negative swing will force us to back down the drive to meet the design defined clipping constraint. Pload = 10^2/(2*110) = 0.455 W Conjugate matching resulted in a 10*log(0.455/4.55) = 10 dB available power hit. Power amplifiers are not designed with conjugate matching in mind. You don't need to re-invent the wheel. Just follow well established principles when doing cookie cutter PA design. The list could go on,... LOL. Given your pattern, I am sure it will. You sighed with content at being offered a "relevent question/statement" Your re-iterative response contains the same (how could it be otherwise?) slack of precision that started this. Want to try again? Not really. The problem isn't precision, it is you can't, or refuse, to comprehend what is being said, which I presume is why you instead write with the most bizarre terms and phrasology that has nothing of import to the topic at hand. You could have as easily expressed what sense they ARE matched, For what seems like the billionth time now: they are load-line matched. ...but instead this time offer what Basis of Matching you are attempting to describe. I've given a didactic example (actually a couple), you just don't--or more likely won't--get it. If you don't like my example, you can refer to Cripps, who is considered one of the preeminant RF PA experts in the world. Even more simplistic is Malvino's discussion on pp177-185 of the first edition ((c) 1968) of "Transistor Circuit Approximations." It is basically a technician level description, so perhaps it is well-suited to you. In academics, load-line theory is presented down to tech level courses and up across to engineering. That some engineers and techs aren't clear on the load-line concept for PA's (or *any* circuit needing a wide symmetrical swing) is notwithstanding. This is the more rigorous approach that eliminates vague descriptions and uses standard terms. If you have to query about what "Basis" means (used by professionals - namely metrologists who can quantify Output Z of all sources) - then we can skip it as a topic out of the reach of amateur discussion. I see you still don't know what impedance is. In any case, it doesn't mean that looking into a properly designed PA output with a network analyzer confirms the conj-match precept, it doesn't. Impedance is a *linear* conception, a portion of linear theory, and again by definition: Z = V/I V and I are sinusoids (phasors). But with power amps, substantial non-linearity exists (destroying the linearity assumption of impedance), thus applying a linearly defined concept to a non-linear milieu is a misapplication. You are attempting, as is Ken, to stuff a square peg down a round hole. Why? The concept is even questionable for the most linear of the power amps: class A. In any case, given real devices with real supplies, the conj-match ideal is next to worthless. While I could agree that the borderline may be fuzzy regarding where and when to drop the impedance notion, it still stands that the concept is not useful in determining how to optimally load an RF PA. At this point you own the conj-match assertion as much as Ken. Prove it! You can't because it is fundamentally incorrect. Note: Again, RF PA's should be load-line matched. Does not qualify as a Basis. Load-line matching is such a basic electronic concept it is unbelievable how oblivious you are to the concept. Read a basic book. Don't rely on me: look it up and do your own design! It is suggestive of one, but because you indiscriminately mix several Basis within your discussions, it is your responsibility to be precise. You just like to hear yourself talk. I've been explicit and precise. You just don't know anything about the elementary electronics principle of load line matching. I presume this is why your comments have zero substantive responsiveness. If you can accomplish this, then we can proceed to review how little it all matters. If you keep ignoring what I've written, and that which is written in elementary electronics texts, you can remain happily ignorant of understanding the simple-basic-fundamental concept presented. Your choice. Barring resolving any of these issues of precise language,...] The guy ignorant of the definition of impedance and that s-domain theory *is* linear circuit theory (and more goodies) is talking about "precise language." Amusing. I notice that you rather enjoy... No, I don't enjoy it at all. Your lack of electronic understanding is dismal, especially given your tone. It would have been a lot easier for me if Ken hadn't made the erroneous statement in the first place and made a correct one instead. That would have been my preferance. ..fruitless jousting with them than challenging my support of Ken's (supposed) statement that you say is your focus: However, responding to the bald statement, I find nothing objectionable about it. That's because you don't understand the difference between impedance matching and ac load line matching. We will leave that as another dead-end. I suspect you will. I already understand it -- you're the one who doesn't. "One of the principal differences between linear RF amplifier design and PA design is that, for optimum power, the output of the device is not presented with the impedance required for a linear conjugate match. That causes much consternation and has been the subject of extensive controversy about the meaning and nature of conjugate matching. It is necessary, therefore, to swallow that apparently unpalatable result as early as possible (Section 1.5), before going on to give it more extended interpretation and analysis (Chapter 2)." -- Cripps, p1 The quote is on Page 1. Swallow it now. Learn something for a change. |
#2
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On Fri, 04 Mar 2005 01:13:39 GMT, "Thomas Magma"
wrote: Wow this is a long thread. Don't really know where I should put my two bits in, but here it goes. I have designed several RF PA sections in the past. 500MHz at about 50W. Pretty easy stuff if you have the right tools and know how to use them. The tools I like using for matching the power output FET is two triple stub tuners. One on the input of the FET and one on the output. So it goes...pre-amp (50 ohm output) - stub tuner - FET - stub tuner - 50 ohm dummy pad - spectrum analyzer. Then just tune the stubs for the performance you desire, these include: efficiency (thermal issues), harmonic content, spurious emissions, load VSWR considerations, cold start, ect. Then remove the FET and look into the triple stub tuners with the network analyzer. Model and duplicate the network out of discrete components that can handle the voltage/power, send the design off to the enviro test lab, and head home early for the day. Cheers, Thomas Hi Thomas, Thanx, your two bits were worth more than the academic plug nickel. This is something that our original poster should hearken to as his needs were obviously production oriented. Bench experience will trump cut-and-paste theory in a heart-beat. However, triple stub is pretty aggressive. How long did it take you to flatten response? 73's Richard Clark, KB7QHC |
#3
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Response is flattened through gain controlling the pre-amp from a look-up
table held in the micro's EEPROM. The alignment procedure is automated using the HB-IP bus from the spectrum analyzer and a computer. The computer/analyzer also looks for harmonic content and spurious emissions during this procedure. Think it takes about ten seconds to do this. "Richard Clark" wrote in message ... On Fri, 04 Mar 2005 01:13:39 GMT, "Thomas Magma" wrote: Wow this is a long thread. Don't really know where I should put my two bits in, but here it goes. I have designed several RF PA sections in the past. 500MHz at about 50W. Pretty easy stuff if you have the right tools and know how to use them. The tools I like using for matching the power output FET is two triple stub tuners. One on the input of the FET and one on the output. So it goes...pre-amp (50 ohm output) - stub tuner - FET - stub tuner - 50 ohm dummy pad - spectrum analyzer. Then just tune the stubs for the performance you desire, these include: efficiency (thermal issues), harmonic content, spurious emissions, load VSWR considerations, cold start, ect. Then remove the FET and look into the triple stub tuners with the network analyzer. Model and duplicate the network out of discrete components that can handle the voltage/power, send the design off to the enviro test lab, and head home early for the day. Cheers, Thomas Hi Thomas, Thanx, your two bits were worth more than the academic plug nickel. This is something that our original poster should hearken to as his needs were obviously production oriented. Bench experience will trump cut-and-paste theory in a heart-beat. However, triple stub is pretty aggressive. How long did it take you to flatten response? 73's Richard Clark, KB7QHC |
#4
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On Fri, 04 Mar 2005 16:47:05 GMT, "Thomas Magma"
wrote: Response is flattened through gain controlling the pre-amp from a look-up table held in the micro's EEPROM. The alignment procedure is automated using the HB-IP bus from the spectrum analyzer and a computer. The computer/analyzer also looks for harmonic content and spurious emissions during this procedure. Think it takes about ten seconds to do this. Hi Thomas, 10 seconds to adjust all 6 stubs? 73's Richard Clark, KB7QHC |
#5
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No the triple stub tuners are only for development. Production boards have
discrete components to form the match network. Power levelling or "flattening the response" is computer adjusting the output power to compensate for the reactive components to ensure a constant output power over the entire band of the radio. We also put in a small temperature compensation coefficient into the EEPROM because the PA tends to put out more power when it is cold. "Richard Clark" wrote in message ... On Fri, 04 Mar 2005 16:47:05 GMT, "Thomas Magma" wrote: Response is flattened through gain controlling the pre-amp from a look-up table held in the micro's EEPROM. The alignment procedure is automated using the HB-IP bus from the spectrum analyzer and a computer. The computer/analyzer also looks for harmonic content and spurious emissions during this procedure. Think it takes about ten seconds to do this. Hi Thomas, 10 seconds to adjust all 6 stubs? 73's Richard Clark, KB7QHC |
#6
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On Fri, 04 Mar 2005 17:39:04 GMT, "Thomas Magma"
wrote: No the triple stub tuners are only for development. Hi Thomas, I thought 10 seconds was awful quick. How long would it take to flatten the response when manually adjusting the triple stub tuners? What merit did you find with triple that could not be found with double stub tuners? 73's Richard Clark, KB7QHC |
#7
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If your amp has to operate over a wide frequency range it is not likely that
you can flatten the response just with stubs. Stubs should be looked at as more single frequency devices than broadband networks. But you can use the stubs to plot out the appropriate impedance curve on the Smith Chart to ensure a flat response when you model in the discretes. I usually just try to get the flatness of the response as close as possible and rely on a software calibration routine to flatten it off. Saves a lot of time. It's my understanding that a triple stub tuner of the right length can reach anywhere on the Smith Chart where as a double stub can not. "Richard Clark" wrote in message ... On Fri, 04 Mar 2005 17:39:04 GMT, "Thomas Magma" wrote: No the triple stub tuners are only for development. Hi Thomas, I thought 10 seconds was awful quick. How long would it take to flatten the response when manually adjusting the triple stub tuners? What merit did you find with triple that could not be found with double stub tuners? 73's Richard Clark, KB7QHC |
#8
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![]() Thomas Magma wrote: No the triple stub tuners are only for development. Production boards have discrete components to form the match network. Power levelling or "flattening the response" is computer adjusting the output power to compensate for the reactive components to ensure a constant output power over the entire band of the radio. We also put in a small temperature compensation coefficient into the EEPROM because the PA tends to put out more power when it is cold. Richard was asking how long it took you to tune the triple stub filters during devolpment. I am curious about the exact nature of the impedance transmformation these devices provided. jk "Richard Clark" wrote in message ... On Fri, 04 Mar 2005 16:47:05 GMT, "Thomas Magma" wrote: Response is flattened through gain controlling the pre-amp from a look-up table held in the micro's EEPROM. The alignment procedure is automated using the HB-IP bus from the spectrum analyzer and a computer. The computer/analyzer also looks for harmonic content and spurious emissions during this procedure. Think it takes about ten seconds to do this. Hi Thomas, 10 seconds to adjust all 6 stubs? 73's Richard Clark, KB7QHC |
#9
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Richard Clark wrote:
On Fri, 04 Mar 2005 01:13:39 GMT, "Thomas Magma" wrote: Wow this is a long thread. Don't really know where I should put my two bits in, but here it goes. I have designed several RF PA sections in the past. 500MHz at about 50W. Pretty easy stuff if you have the right tools and know how to use them. The tools I like using for matching the power output FET is two triple stub tuners. One on the input of the FET and one on the output. So it goes...pre-amp (50 ohm output) - stub tuner - FET - stub tuner - 50 ohm dummy pad - spectrum analyzer. Then just tune the stubs for the performance you desire, these include: efficiency (thermal issues), harmonic content, spurious emissions, load VSWR considerations, cold start, ect. Then remove the FET and look into the triple stub tuners with the network analyzer. Model and duplicate the network out of discrete components that can handle the voltage/power, send the design off to the enviro test lab, and head home early for the day. Cheers, Thomas Hi Thomas, Thanx, your two bits were worth more than the academic plug nickel. This is something that our original poster should hearken to as his needs were obviously production oriented. I doubt you understand what he wrote. I can't fathom why you would be concerned with the OP when your own difficulties are so acute. Bench experience will trump cut-and-paste theory in a heart-beat. How would you know? However, triple stub is pretty aggressive. How long did it take you to flatten response? How long will it take you to figure out that he wrote not a wisp of a word on what the "output-Z" of the amplifier is? He did write that he determines how the amp was loaded to acheive power, something I've been saying is the prime concern. |
#10
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Hi gwhite,
I would have to agree with you on most everything you have said through this thread. I once saw my boss (with his "PHD") try to model and match a power amp based on the small signal parameters off the datasheet. He insisted that the stated input and output impedances were characteristic parasitics of that amp and wouldn't change between a small or large signal. It was kind of pathetic to watch him struggle for over a month on the matching network, and I think he had resorted to guessing in the end. I've often questioned why manufactures put small signal parameters on their datasheets? Makes no sense to me. Even if they do publish some large signal parameters it is unlikely to be the exact same mode of operation that you need for your project. Playing with triple stub tuners on PA's has shown me that there are many combinations of input and output impedances that appear to give similar results at any one frequency, but give different results at others frequencies. So it's a matter of finding the input and output impedance that give you adequate performance over the entire scope of your project. Thomas "gwhite" wrote in message ... Richard Clark wrote: On Fri, 04 Mar 2005 01:13:39 GMT, "Thomas Magma" wrote: Wow this is a long thread. Don't really know where I should put my two bits in, but here it goes. I have designed several RF PA sections in the past. 500MHz at about 50W. Pretty easy stuff if you have the right tools and know how to use them. The tools I like using for matching the power output FET is two triple stub tuners. One on the input of the FET and one on the output. So it goes...pre-amp (50 ohm output) - stub tuner - FET - stub tuner - 50 ohm dummy pad - spectrum analyzer. Then just tune the stubs for the performance you desire, these include: efficiency (thermal issues), harmonic content, spurious emissions, load VSWR considerations, cold start, ect. Then remove the FET and look into the triple stub tuners with the network analyzer. Model and duplicate the network out of discrete components that can handle the voltage/power, send the design off to the enviro test lab, and head home early for the day. Cheers, Thomas Hi Thomas, Thanx, your two bits were worth more than the academic plug nickel. This is something that our original poster should hearken to as his needs were obviously production oriented. I doubt you understand what he wrote. I can't fathom why you would be concerned with the OP when your own difficulties are so acute. Bench experience will trump cut-and-paste theory in a heart-beat. How would you know? However, triple stub is pretty aggressive. How long did it take you to flatten response? How long will it take you to figure out that he wrote not a wisp of a word on what the "output-Z" of the amplifier is? He did write that he determines how the amp was loaded to acheive power, something I've been saying is the prime concern. |
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