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Keith Dysart wrote:
It seems to me that if connecting a -j567 impedance produces a certain response, it should not matter how that -j567 impedance is produced. Consider the following cases: (1) - produce the -j567 with a lumped capacitor (2) - produce the -j567 with 10 degrees of 100 ohm line (3) - produce the -j567 with 46.6 degrees of 600 ohm line The claim appears to be that despite the 43.4 degrees of 600 ohm line being terminated in the exact same -j567 impedance in all cases, the phase shift experienced at the interface is different in each case. They are terminated in the same value of impedance but they are not terminated in identical impedances. Please see the IEEE Dictionary for the three different definitions of impedance. Each case involves a different reflection coefficient at the -j567 point. (I added a number to each case above.) (1) involves an *impedor* with a reflection coefficient of 1.0 at -93.2 degrees when connected to the 600 ohm line. The reflected wave at the feedpoint lags the forward wave by 43.4 + 93.2 + 43.4 = 180 degrees. The impedance is a real impedor, not a virtual impedance. (2) involves an impedance discontinuity with a reflection coefficient of -0.7143. With 10 degrees of 100 ohm line, the reflected wave lags the forward wave by 2(43.4 + 36.6 + 10) = 180 degrees. The phase shift at the discontinuity is 36.6 degrees each way. The impedance is caused by superposition of component waves at the impedance discontinuity. (3) with 46.6 degrees of 600 ohm line, the reflected wave lags the forward wave by 2(43.4 + 0 + 46.6) = 180 degrees. The phase shift at the 600 to 600 ohm junction is zero. The reflection coefficient at the 600 to 600 ohm junction is 0, different from (1) and (2) above. The impedance is completely virtual and thus cannot cause anything. -- 73, Cecil http://www.w5dxp.com |
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