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3.23: Single-Stub Matching
https://phys.libretexts.org/Bookshelves/Electricity_and_Magnetism/Electromagnetics_I_(Ellingson)/03%3A_Transmission_Lines/3.23%3A_Single-Stub_Matching
(unable to fetch text document from uri [status: 403 (Forbidden)])
3.23: Single-Stub Matching
https://phys.libretexts.org/Courses/Berea_College/Electromagnetics_I/03%3A_Transmission_Lines/3.23%3A_Single-Stub_Matching
Since parallel reactance matching is most easily done using admittances, [admittance] it is useful to express $Z_{i n}(l)=+j Z_{0} \tan \beta l$ and $Z_{i n}(l)=-j Z_{0} \cot \beta l$ (input imped...Since parallel reactance matching is most easily done using admittances, [admittance] it is useful to express $Z_{i n}(l)=+j Z_{0} \tan \beta l$ and $Z_{i n}(l)=-j Z_{0} \cot \beta l$ (input impedance of an open- and short-circuited stub, respectively, from Section 3.16) in terms of susceptance: $B_p = -Y_{02} \cot\left(\beta_2 l_2\right) ~~\mbox{short-circuited stub} \nonumber$ $B_p = +Y_{02} \tan\left(\beta_2 l_2\right) ~~\mbox{open-circuited stub} \nonumber$ As in the main line, th…

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