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3.18: Measurement of Transmission Line Characteristics
https://phys.libretexts.org/Courses/Berea_College/Electromagnetics_I/03%3A_Transmission_Lines/3.18%3A_Measurement_of_Transmission_Line_Characteristics
and when a transmission line is terminated in an open circuit, the input impedance is $Z_{in}^{(OC)} = -jZ_0 \cot\beta l \nonumber$ Observe what happens when we multiply these results together: \[Z...and when a transmission line is terminated in an open circuit, the input impedance is $Z_{in}^{(OC)} = -jZ_0 \cot\beta l \nonumber$ Observe what happens when we multiply these results together: $Z_{in}^{(SC)} \cdot Z_{in}^{(OC)} = Z_0^2 \nonumber$ that is, the product of the measurements $Z_{in}^{(OC)}$ and $Z_{in}^{(SC)}$ is simply the square of the characteristic impedance.

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