Home |
Search |
Today's Posts |
#15
![]() |
|||
|
|||
![]()
"walt" wrote in news:1173278086.390893.310040@
30g2000cwc.googlegroups.com: On Mar 3, 4:37 am, Richard Clark wrote: On Sat, 3 Mar 2007 00:10:21 +0000, Ian White GM3SEK .... I've been reading this thread with interest, but the discussions appear to be only academically related. On the other hand, I've made measurements that prove the sailent points of these academic discussions. These measurements were made since those reported in Reflections 2, and will appear in Reflections 3. However, they are available on my web page at www.w2du.com. Go to 'Preview of Chapters from Reflections 3' and click on Chapter 19A. You may want to disregard the first portion of the chapter, which is an epilog to Bruene's fiction concerning the conjugate match. The pertinent portion here is that which reports in detail the step-by- step procedure in measuring the output impedance of a Kenwood TS-830S transceiver feeding a reactive-impedance load. With a careful review of these steps I'm sure you'll find empirical proof of the academics appearing in the previous posts. Hi Walt, I have read your document with interest, and will reread it a couple of times yet. The measurements are interesting, and on a first read, appear consistent and in agreement with how things work as I understand it. However, I don't believe any of your measurents actually reveal the source impedance. You have shown the impact of the changed load on the transmitter. You have demonstrated admirably the transformation of the two external loads to the load seen by the plate(s), and you have shown what the transmitter looks like from the antenna socket with a resistor in place of the valves. So, IMHO, the promise "The output source resistance of the amplifier in this condition will later be shown to be 50 ohms" is not fulfilled. It is my view that the statement "Because the amplifier was adjusted to deliver the maximum available power of 100 watts prior to the resistance measurement, resistance RLP looking into the plate (upstream from the network terminals) is also approximately 1400 ohms" is not proven. If we were to view the plate as a generator, and the pi network as a lossless flexible variable impedance transformer, and you were to adjust the pi network for maximum power transfer, that would imply that the impedance loading the generator was the complex conjugate of its equivalent series resistance... IF and ONLY IF the generator can be accurately represented by an equivalent series circuit of a fixed voltage generator and fixed equivalent series impedance. The question is can the plate (or the whole transmitter for that matter) be accurately replaced by an equivalent series circuit of a fixed voltage generator and fixed equivalent series resistance (independent of load). How would such a simple model deal with the case of a transmitter that at maximum power output is close to voltage saturation (ie cannot develop more output voltage) and close to current saturation (ie cannot develop more output current)? These non-linear behaviours close to operating point are not captured in a simple linear equivalent circuit. Owen |
Thread Tools | Search this Thread |
Display Modes | |
|
|
![]() |
||||
Thread | Forum | |||
FS: Collins 32V-3 HF Transmitter NICE!!! | Boatanchors | |||
Narrow lobe of a yagi | Antenna | |||
FCC: Broadband Power Line Systems | Policy | |||
Wanted: Power Supply for TR-4C | Homebrew | |||
Power vs Mode (The fundamentals) | CB |