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#1
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W2DU's Reflections III is now available from CQ Communications,Inc.
On May 24, 6:15*pm, Keith Dysart wrote:
This may be the root of my disagreement. Certainly the output can be an arbitrarily perfect sine wave, but this simply depends on the characteristics of the filter and not on whether the system is linear. Since anything except a class-A amplifier is non-linear and since we are talking about linear analysis, it seems we need to locate a point in the system where V is a sine wave, I is a sine wave, and V/I is the constant impedance at that point. IMO, that is the first point at which we can use a linear math analysis and maybe that point is what Walt is talking about. It's certainly not going to be the plate of a class-C amplifier and it may not even be the load-line of the class-C amplifier. There is probably some point in an otherwise non-linear system where a linear analysis becomes possible. I think that point is what Walt considers to be the linear source point, wherever that point might be located. In fact, here is my personal take on the subject. Given an antenna system that presents 50+j0 ohms looking into 50 ohm coax, the internal impedance of the source doesn't matter. For any voltage source, irrespective of the source impedance, if reflected energy doesn't reach the source, the source impedance doesn't matter (except for efficiency). Seems to me, the highest efficiency would be achieved by a source with zero ohms of source impedance. -- 73, Cecil, w5dxp.com |
#2
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W2DU's Reflections III is now available from CQ Communications,...
Cecil Moore, W5DXP wrote:
"Seems to me, the highest efficiency would be achieved by a source with zero source impedance." Me too, but zero source impedance does not match the load as required for maximum power transfer. The best combination is then a source impedance matching the load and which is also pracrically lossless. The Class C amplifier does this by acting as a switch which is infinite in impedance when open during a large part of the RF cycle and a near short circuit to a low impedance (near zero Z) D.C. power source for the short part of the RF cycle it is switched on. It is the time averaged impedance which counts. Is this linear? No way, but the tank circuit is able to remove the harmonics and turn current pulses into a low distortion sine wave. Efficiency? Terman says on page 450 of his 1955 opus that Class C eddiciency is typically 60% to 80%. Compare that with 50% efficiency in a Class A amplifier. Best regards, Richard Harrison, KB5WZI |
#3
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W2DU's Reflections III is now available from CQCommunications,...
On May 25, 12:32*am, (Richard Harrison)
wrote: Cecil Moore, W5DXP wrote: "Seems to me, the highest efficiency would be achieved by a source with zero source impedance." Me too, but zero source impedance does not match the load as required for maximum power transfer. It seems to me that much too much is made of 'maximum power transfer' in the RF world. In the world of 50 and 60 Hz, where significantly more energy is moved, 'maximum power transfer' is never mentioned. Efficiency is much more of interest. For the most part, 'maximum power transfer' is just an interesting ideosyncracy of linear circuit theory. ....Keith |
#4
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W2DU's Reflections III is now available from CQCommunication...
Keith Dysart wrote:
"For the most part, "maximum power transfer is just an interesting ideosyncracy of linear circuit theory." In the world of 50 and 60 Hz, we don`t want all the power plant can supply when we flip on a light switch. The RF world is usually different. Maximum power transfer only occurs when source and load match conjugately, and the match proves the load and source impedances are equals. It is well known and easily shown that a match results in maximum power transfer. If one has a 100-watt transmitter he probably wants 100 watts out of it sometimes and may only be able to do so when his antenna is matched to his transmitter, Maxumum power treansfer is more than an "interesting ideosyncracy". Best regards, Richard Harrison, KB5WZI |
#5
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W2DU's Reflections III is now available from CQ Communication...
Richard Harrison wrote:
Keith Dysart wrote: "For the most part, "maximum power transfer is just an interesting ideosyncracy of linear circuit theory." In the world of 50 and 60 Hz, we don`t want all the power plant can supply when we flip on a light switch. The RF world is usually different. Maximum power transfer only occurs when source and load match conjugately, and the match proves the load and source impedances are equals. It is well known and easily shown that a match results in maximum power transfer. . . . It's also easily shown that it doesn't. Consider a 10 volt voltage source having a 50 ohm source resistance, feeding a 50 ohm resistive load. Power at the load is 0.5 watt, is it not? Reduce the source impedance to 10 ohms. Now what is the power dissipated in the load? Is it greater or less than it was when the source and load impedances were matched? Roy Lewallen, W7EL |
#6
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W2DU's Reflections III is now available from CQ Communication...
On May 26, 6:20*pm, Roy Lewallen wrote:
Richard Harrison wrote: Keith Dysart wrote: "For the most part, "maximum power transfer is just an interesting ideosyncracy of linear circuit theory." In the world of 50 and 60 Hz, we don`t want all the power plant can supply when we flip on a light switch. The RF world is usually different. Maximum power transfer only occurs when source and load match conjugately, and the match proves the load and source impedances are equals. It is well known and easily shown that a match results in maximum power transfer. . . . It's also easily shown that it doesn't. Consider a 10 volt voltage source having a 50 ohm source resistance, feeding a 50 ohm resistive load. Power at the load is 0.5 watt, is it not? Reduce the source impedance to 10 ohms. Now what is the power dissipated in the load? Is it greater or less than it was when the source and load impedances were matched? Roy Lewallen, W7EL But Roy, consider that the source resistance remains constant at 10 ohms. Then what load resistance will absorb the most power? The answer is 10 ohms. Any value of load resistance greater or less than 10 ohms will result in less power delivered. I don't believe it's fair to change the source resistance when dealing with the Maximum Power Transfer Theorem. In your example with a source resistance of 10 ohms and a load resistance of 50 ohms the power delivered will be 1.39 watts. But when the load resistance is 10 ohms with the same source resistance the power delivered is 2.5 watts. As I said above, if the load resistance is either greater or less than 10 ohms the power delivered will be less than 2.5 watts. Thus when the source resistance is constant the maximum power will be delivered when the load is matched to the source. Nes pa? Walt |
#7
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W2DU's Reflections III is now available from CQ Communication...
walt wrote:
But Roy, consider that the source resistance remains constant at 10 ohms. Then what load resistance will absorb the most power? The answer is 10 ohms. Any value of load resistance greater or less than 10 ohms will result in less power delivered. I don't believe it's fair to change the source resistance when dealing with the Maximum Power Transfer Theorem. In your example with a source resistance of 10 ohms and a load resistance of 50 ohms the power delivered will be 1.39 watts. But when the load resistance is 10 ohms with the same source resistance the power delivered is 2.5 watts. As I said above, if the load resistance is either greater or less than 10 ohms the power delivered will be less than 2.5 watts. Thus when the source resistance is constant the maximum power will be delivered when the load is matched to the source. Nes pa? Walt Of course, I know that, and I would hope anyone with even very basic electrical circuit analysis knowledge does. And anyone with that knowledge should state as you have, "FOR A GIVEN SOURCE IMPEDANCE, maximum power transfer occurs when the source and load impedances are matched (i.e., the load impedance is the complex conjugate of the source impedance)," which is true. But the statement which was made was that "Maximum power transfer occurs when the source and load impedances are matched." This is NOT true, as the example demonstrates. It's an important distinction. Instead of declaring what's "fair" and what isn't with regard to changing source and load impedances, the maximum power transfer theorem should be stated correctly, in a way which makes it true. Roy Lewallen, W7EL |
#8
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W2DU's Reflections III is now available from CQCommunication...
Roy Lewallen wrote:
"Reduce the source imperance to 10 ohms." FOUL! In the case of a 10-ohm internal source, the load which extracts maximum power is 10 ohms. Best regards, Richard Harrison, KB5WZI |
#9
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W2DU's Reflections III is now available from CQ Communication...
I stand by my position that when the source is an RF power amplifier,
and when all the available power is transferred from the source to the load, the source impedance is the conjugate of the load impedance. In a similar instance, if the load is a pure resistance, the source resistance equals the load resistance. And referring to a statement Dysart made concerning plate resistance, Rp, it must be understood that in Class AB, B and C amplifiers, Rp is NOT the source resistance. In those amplifiers the effect of Rp is a negative feedback that reduces the effect of plate-current change resulting from a change in grid voltage, thus reducing the power output compared to what the output would be if Rp were absent. Compensation for the power lost to Rp is accomplished by simply increasing the grid drive. Consequently, Rp plays no part in achieving a conjugate match at the junction of the network-output and the load. Although lossless elements are required to achieve a perfect conjugate match in both directions, a perfect conjugate match is obtained in the forward direction with real elements when all available power is being delivered to the load. This condition is verified in data presented in Chapter 24 of Reflections 3. Walt, W2DU |
#10
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W2DU's Reflections III is now available from CQCommunications,...
On May 24, 11:32*pm, (Richard Harrison)
wrote: Cecil Moore, W5DXP wrote: "Seems to me, the highest efficiency would be achieved by a source with zero source impedance." Me too, but zero source impedance does not match the load as required for maximum power transfer. A 60 Hz Power Generation Plant operates at high efficiency, not at the maximum power transfer point. If they were 50% efficient, they would go out of business. (That's what Edison expected.) Why is maximum power transfer desirable in ham transmitters? Is such a design the highest power/cost ratio? Is it possible to build an output amp with a 10 ohm source impedance designed to be 80% efficient? 1 ohm source impedance designed to be 98% efficient? Is co$t the driving parameter? -- 73, Cecil, w5dxp.com |
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