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On 27 abr, 23:18, Cecil Moore wrote:
On Apr 27, 1:43*pm, Wimpie wrote: In other words, the amplifier sees a constant VSWR, but with changing phase. Small frequency difference results in slow phase change of VSWR. From the IEEE Dictionary: "impedance - (1)(A) The corresponding impedance function with p replaced by jw in which w is real. Note: Definitions (A) and (B) are equivalent. (1)(B) The ratio of the phasor equivalent of a steady- state sine wave voltage ... to the phasor equivalent of a steady-state sine wave current ... (1)(C) A physical device or combination of devices whose impedance as defined in definition (A) or (B) can be determined. Note: This sentence illustrates the double use of the word impedance ... Definition (C) is a second use of 'impedance' and is independent of definitions (A) and (B)." The pinging experiment seems to be measuring a physical impedance (1) (C) the nature of which is unclear. When the amplifier is outputting power, it seems that the source impedance would be a V/I ratio (1)(B) which doesn't respond to incoherent signals. Seems to me, you guys are pinging something other than the source impedance. -- 73, Cecil, w5dxp.com "Halitosis is better than no breath at all.", Don, KE6AJH/SK Hello Cecil, You may try to figure out how the signal injection method functions (it is a form of active load pulling). Can you agree with: it doesn't matter whether: -power reflect towards the amplifier is caused by load mismatch, or -power is sent towards the amplifier by means of a phase synchronized source. This source is phase synchronized with the PA's exciter, so we have a steady state system. We assume small load mismatch (or low injected power towards the PA) so that the operating point of the PA just changes slightly (to allow linear approximation). Now we insert a coupler between the amplifier and the load. This coupler will measure the forward voltage generated by the PA, plus the reflected part of the voltage that originates from the phase synchronised source. Depending on the phase relationship, it can be more or less then the forward voltage of the PA. If the PA shows 50 Ohms, the coupler's output would not change due to the signal injection (as no signal is reflected by the PA). We note the forward coupler's output voltage (both phase and amplitude). Now we change the phase relationship between the exciter and the source that transmits some power toward the PA. Lets change 180 degrees and keep the amplitude the same. We again note the coupler's output voltage (both phase and amplitude). The voltage that is reflected by the PA equals half the complex voltage change because of the phase change. Off course you have to correct the readings because of the coupler loss. If you know the signal that is send toward the PA, you can now calculate the complex output impedance of the PA for small load change around 50 Ohms. Instead of changing the phase of the source manually, you can do that continuously and note the couplers output continuously. If you change the phase of a signal continuously (with certain constant rad/s), the result is a decrease or increase of frequency. Assuming some reflection by the PA, the complex output from coupler rotates around a certain point. That certain point is the result of the PA's output power and the rotating vector is the result from the injected signal that is reflected by the PA (back towards the load). With a VSA you can discriminate between the voltage component from the PA itself and the reflected component (with slightly different frequency). With a normal spectrum analyser, you can only determine the magnitude of the PA's reflection coefficient (or VSWR as you like). Given the dynamic range of today's equipment, you can inject a very low level signal that may mimic load mismatch well below VSWR = 1.1. With respect to the impedance concept, we as amateurs do not use steady state signals, as they contain no information. We modulate them and are still using the impedance concept, despite the definitiones you showed. As long as the signal that is injected is well within the pass band of the PA and it sufficiently low to allow linear approximation, the concept of superposition and concept of impedance still holds. But if you feel more confident with the manual phase change, or using two known loads with known slight mismatch, I have nothing against it. But if you have a VSA, some couplers and signal source at hand, it may save lots of time. With kind regard, Wim PA3DJS www.tetech.nl |
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