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#21
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Henry wrote,
I know that any power not dissipated by an antenna is reflected back to the transmitter. Then the transmitter "reflects" this reflection back to antenna, ad nauseum until its all gone. I also know that a short or an open is required to reflect power and I'm searching for which it is, an open or a short. I'm inclined to think it's a virtual open but I'm at a loss to understand that and I wonder if someone has a good explanation or analogy and some math wouldn't hurt. tnx Hank WD5JFR This post is guaranteed to get Cecil revivified. Here's a hint: quit thinking solely in terms of power, that's for fellows who want to explain how it all works without going into any of the complicated details. Get an undergraduate physics text that discusses waves, and read it, or, better yet, take a class. Take all explanations you read in amateur publications with a grain of salt. After you've done this, you still won't be able to argue with Cecil, because that requires an extensive knowledge of the moronic, unfair, and downright pathalogical debating techniques of which Cecil is a master. But, it will be harder for you to fall for some of the crackpot ideas you're liable to read on this newsgroup, and it will give you something to think about when sipping your after-dinner port. 73, Tom Donaly, KA6RUH |
#22
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Tam/WB2TT wrote:
I am not quite sure what you are saying. But, I ran a SPICE simulation of the following: 1V 1MHz source with resistor R0 feeding a 50 Ohm 250 ns transmission line shorted at the far end. Independent of R0, in steady state the voltage at the input end of the transmission line will be 1V. The effect of R0 is to limit how long it takes to reach steady state. For R0 = 50 Ohms, it is one cycle; for R0 = 500 Ohms, it is about 8 cycles, as eyeballed off the waveform display. Does SPICE report the steady-state forward and reflected waves or just the superposition of those two waves? We all know what they look like when superposed. The question is whether the identity of the forward and reflected waves disappear after they are superposed. To the best of my knowledge, the very existence of standing waves requires the existence of a forward- traveling wave and a rearward-traveling wave. I have asked for examples of standing waves void of rearward- traveling waves and none has been forthcoming. -- 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 100,000 Newsgroups - 19 Different Servers! =----- |
#23
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Tdonaly wrote:
This post is guaranteed to get Cecil revivified. Here's a hint: quit thinking solely in terms of power, that's for fellows who want to explain how it all works without going into any of the complicated details. Like Hewlett Packard in their AN 95-1 publication? "Another advantage of the s-parameters springs from the simple relationship between the variables a1, a2, b1, and b2, and *various power waves*. ... The previous four equations show that s-parameters are simply related to power gain and mismatch loss, quantities which are often of more interest than the corresponding voltage functions." -- 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 100,000 Newsgroups - 19 Different Servers! =----- |
#24
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I just want to know the reflection physics in the Tx, no antenna tuner, just
a mismatched antenna. I recall no pysics book that tell me how the reflection sees the transmitter. 73 Hank WD5JFR There are no stupid questions, just stupid people asking! "Tdonaly" wrote in message ... Henry wrote, I know that any power not dissipated by an antenna is reflected back to the transmitter. Then the transmitter "reflects" this reflection back to antenna, ad nauseum until its all gone. I also know that a short or an open is required to reflect power and I'm searching for which it is, an open or a short. I'm inclined to think it's a virtual open but I'm at a loss to understand that and I wonder if someone has a good explanation or analogy and some math wouldn't hurt. tnx Hank WD5JFR This post is guaranteed to get Cecil revivified. Here's a hint: quit thinking solely in terms of power, that's for fellows who want to explain how it all works without going into any of the complicated details. Get an undergraduate physics text that discusses waves, and read it, or, better yet, take a class. Take all explanations you read in amateur publications with a grain of salt. After you've done this, you still won't be able to argue with Cecil, because that requires an extensive knowledge of the moronic, unfair, and downright pathalogical debating techniques of which Cecil is a master. But, it will be harder for you to fall for some of the crackpot ideas you're liable to read on this newsgroup, and it will give you something to think about when sipping your after-dinner port. 73, Tom Donaly, KA6RUH |
#25
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Henry Kolesnik wrote:
I just want to know the reflection physics in the Tx, no antenna tuner, just a mismatched antenna. I recall no pysics book that tell me how the reflection sees the transmitter. The reflected waves obey the laws of physics. The kicker is that we don't know (and apparently cannot directly measure) the source impedance. What the reflections can do is modify the designed-for load line through superposition of the forward and reflected waves. Modification of the designed-for load line is not desirable and, if unprotected, can cause over-voltage, over-current, or phase problems. -- 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 100,000 Newsgroups - 19 Different Servers! =----- |
#26
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OK, if we shine a flashlight at a mirror the light bounces back and what
ever is caught by the reflector will be reflected. Take away the reflector and the reflection just keeps going. If someone can tell me what the hot filament does perhaps I can understand what happens in the finals, or whatever. tnx Hank WD5JFR "Cecil Moore" wrote in message ... Henry Kolesnik wrote: I just want to know the reflection physics in the Tx, no antenna tuner, just a mismatched antenna. I recall no pysics book that tell me how the reflection sees the transmitter. The reflected waves obey the laws of physics. The kicker is that we don't know (and apparently cannot directly measure) the source impedance. What the reflections can do is modify the designed-for load line through superposition of the forward and reflected waves. Modification of the designed-for load line is not desirable and, if unprotected, can cause over-voltage, over-current, or phase problems. -- 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 100,000 Newsgroups - 19 Different Servers! =----- |
#27
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Henry Kolesnik wrote:
OK, if we shine a flashlight at a mirror the light bounces back and what ever is caught by the reflector will be reflected. Take away the reflector and the reflection just keeps going. If someone can tell me what the hot filament does perhaps I can understand what happens in the finals, or whatever. The hot filament provides a source of electrons. How many electrons are emitted depends on the instantaneous voltages on the other elements, the plate and grids. Reflected waves have an effect on those instantaneous voltages but IMO, there's not much sense in pursuing the "filament" line of reasoning. -- 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 100,000 Newsgroups - 19 Different Servers! =----- |
#28
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It's true in the case of transmission lines that there are standing
waves and reflections but, unfortunately, this concept has somehow come to dominate and confuse the concept of matching a tranmitter to an antenna -- a generator to a load. Like in many areas of science, mathematicians and scientists often find convenient ways to mathematically describe and predict physical phenomenon that hinders, even misleads, the understanding of how it actually works. If you leave out the complex part of impedences for the moment and think of 100 volt generator that has a 50 ohm internal impedance driving a 50 ohm load, current is 1 amp and the power dissipated by the load is 50 watts. There is also 50 watts dissipated by the generator's internal impedance, for a total of 100 watts dissipated by the entire system. Therefore, the "available" power for this generator is 50 watts. Maximum available I^2*R power only occurs when the load impedance is equal to the generator's characteristic impedance, 50 ohms (do the math). Any load impedance higher or lower, ALWAYS produces less "available" power. Herein lies one of the big problems with the "reflection" definition, conceptually. The generator (transmitter) is not a constant-power device. When a manufacturer says that it's XYZ transmitter produces 100 watts, it only produces (has available) 100 watts (after internal dissipation) into a 50 ohm load. Any other load *always* produces less available power, due to simple I^2*R laws. It has nothing to do with reflections or standing waves, although, mathmatically, reflection formulas accurately describe it. A couple of examples using a 100 volt constant voltage generator and an internal impedance (RG) of 50 ohms: 1) Load (RL) = 50 ohms. Current = 100 / (50 + 50) = 1 amp Power dissipated in RL (PL) = (1)^2*50 = 50 watts Power dissipated in RG (PG) = (1)^2*50 = 50 watts SWR = RL/RG = PL/PG = 1:1 2) Load (RL) = 100 ohms. Current = 100 / (50 + 100) = .667 amp Power dissipated in RL (PL) = (.667)^2*100 = 44.5 watts Power dissipated in RG (PG) = (.667)^2*50 = 22.25 watts SWR = RL/RG = PL/PG = 2:1 3) Load (RL) = 25 ohms. Current = 100 / (50 + 25) = 1.34 amp Power dissipated in RL (PL) = (1.34)^2*25 = 44.9 watts Power dissipated in RG (PG) = (1.34)^2*50 = 89.8 watts SWR = RG/RL = PG/PL = 2:1 Notice that the total power dissipated in all three examples is different. The transmitter is NOT a constant-power source, but it's also not a unlimited power source and has operational limits. Therefore, what is commonly called "reflected power" is power that never leaves the transmitter and is dissipated as heat by the transmitter's internal 50 ohm impedance (if the transmitter's design doesn't prematurely shut down first). Al "Henry Kolesnik" wrote in message ... I know that any power not dissipated by an antenna is reflected back to the transmitter. Then the transmitter "reflects" this reflection back to antenna, ad nauseum until its all gone. I also know that a short or an open is required to reflect power and I'm searching for which it is, an open or a short. I'm inclined to think it's a virtual open but I'm at a loss to understand that and I wonder if someone has a good explanation or analogy and some math wouldn't hurt. tnx Hank WD5JFR |
#29
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alhearn wrote:
Herein lies one of the big problems with the "reflection" definition, conceptually. That's why I often resort to a signal generator with a circulator/load to illustrate my point. That signal generator *is* a constant power source. Therefore, what is commonly called "reflected power" is power that never leaves the transmitter and is dissipated as heat by the transmitter's internal 50 ohm impedance (if the transmitter's design doesn't prematurely shut down first). You can mount an argument that if the source doesn't see its source impedance, then there is a reflection at that internal mismatch. But that's not what is commonly called reflected power. When we talk about reflected power on this newsgroup, we are usually referring to the forward power rejected by a mismatch between the transmission line Z0 and the antenna impedance (associated with mismatch loss). In a typical ham radio antenna system, the "lost" reflected power is forced to engage in destructive interference at the tuner and thus joins the forward power wave. -- 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 100,000 Newsgroups - 19 Different Servers! =----- |
#30
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I thought filaments produced photons/light waves as well. You took me to
light now you want to leave! Come on I just want a good basic understand on what it is the the Tx reflects the power , how it does it and a little simple math. My dad used to say if you can't explain something you think you know to someone else it might because you don't understand it yourself or lack command of the language. In this case for me it's both. 73 Hank WD5JFR "Cecil Moore" wrote in message ... Henry Kolesnik wrote: OK, if we shine a flashlight at a mirror the light bounces back and what ever is caught by the reflector will be reflected. Take away the reflector and the reflection just keeps going. If someone can tell me what the hot filament does perhaps I can understand what happens in the finals, or whatever. The hot filament provides a source of electrons. How many electrons are emitted depends on the instantaneous voltages on the other elements, the plate and grids. Reflected waves have an effect on those instantaneous voltages but IMO, there's not much sense in pursuing the "filament" line of reasoning. -- 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 100,000 Newsgroups - 19 Different Servers! =----- |
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