In calibration for measurement and in measurement at RF frequencies, high-Z
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is far more difficult than a short or proper 50-ohm termination. Take 144 MHz and assume you are attempting to measure 1 kohm. There will always be present roughly 0.5 to 1 pf in the measurement. At 144 MHz, 0.5 pF = -j2210 ohms. This is over twice the real part even at 0.5 pF - a very small capacitor. True, the output impedance (if you will, resistance plus a small amount of several pF of capacitance) of an HF tube amplifier is very high, between 1000 and 4000 ohms (+/-). The pi-L network between the tube plates and the output to the antenna feedline matches that high-Z (and renders pure resistance) to 50-ohms. That impedance is not measured with a VNA but rather but by using standard Ohm's Law based calculations specifically tailored for determining the values of the matching network to enable maximum power transfer. 450 ohm ladder line is a real differential transmission line as is 300-ohm TV twin lead as are long parallel close-spaced ribbons of copper strip as are parallel copper traces on opposing layers of a PC board. I use parallel open wire transmission line between my home brew L-network matching network (a.k.a., "antenna tuner" - it does NOT 'tune' the antenna!!) and the feed point of my 450-foot long doublet. Works great as a relatively lossless transmission line and withstands high SWR with insignificant additional loss. Dave - W?LEV On Mon, Feb 17, 2020 at 3:47 PM Nels Nelsen <nels.nelsen@...> wrote:
My tube amplifier takes exception to your statement: --
*Dave - W?LEV* *Just Let Darwin Work* *Just Think* |