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3.15: Input Impedance of a Terminated Lossless Transmission Line
https://phys.libretexts.org/Bookshelves/Electricity_and_Magnetism/Electromagnetics_I_(Ellingson)/03%3A_Transmission_Lines/3.15%3A_Input_Impedance_of_a_Terminated_Lossless_Transmission_Line
Since the argument of the complex exponential factors is $2\beta l$ , the frequency at which $Z_{in}(l)$ varies is $\beta/\pi$ ; and since $\beta=2\pi/\lambda$ , the associated period is \(\lambd...Since the argument of the complex exponential factors is $2\beta l$ , the frequency at which $Z_{in}(l)$ varies is $\beta/\pi$ ; and since $\beta=2\pi/\lambda$ , the associated period is $\lambda/2$ .
3.15: Input Impedance of a Terminated Lossless Transmission Line
https://phys.libretexts.org/Courses/Berea_College/Electromagnetics_I/03%3A_Transmission_Lines/3.15%3A_Input_Impedance_of_a_Terminated_Lossless_Transmission_Line
Since the argument of the complex exponential factors is $2\beta l$ , the frequency at which $Z_{in}(l)$ varies is $\beta/\pi$ ; and since $\beta=2\pi/\lambda$ , the associated period is \(\lambd...Since the argument of the complex exponential factors is $2\beta l$ , the frequency at which $Z_{in}(l)$ varies is $\beta/\pi$ ; and since $\beta=2\pi/\lambda$ , the associated period is $\lambda/2$ .

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