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    • https://phys.libretexts.org/Courses/Berea_College/Electromagnetics_I/03%3A_Transmission_Lines/3.08%3A_Wave_Propagation_on_a_TEM_Transmission_Line
      We first define real-valued quantities α and β to be the real and imaginary components of γ; i.e., αRe{γ} \[\beta \tr...We first define real-valued quantities α and β to be the real and imaginary components of γ; i.e., αRe{γ} βIm{γ} and subsequently γ=α+jβ Then we observe e±γz=e±(α+jβ)z=e±αz e±jβz It may be easier to interpret this expression by reverting to the time …
    • https://phys.libretexts.org/Bookshelves/Electricity_and_Magnetism/Electromagnetics_I_(Ellingson)/03%3A_Transmission_Lines/3.08%3A_Wave_Propagation_on_a_TEM_Transmission_Line
      We first define real-valued quantities α and β to be the real and imaginary components of γ; i.e., αRe{γ} \[\beta \tr...We first define real-valued quantities α and β to be the real and imaginary components of γ; i.e., αRe{γ} βIm{γ} and subsequently γ=α+jβ Then we observe e±γz=e±(α+jβ)z=e±αz e±jβz It may be easier to interpret this expression by reverting to the time …
    • https://phys.libretexts.org/Courses/Kettering_University/Electricity_and_Magnetism_with_Applications_to_Amateur_Radio_and_Wireless_Technology/21%3A_Electrical_Transmission_Lines/21.10%3A_Wave_Propagation_on_a_Transmission_Line
      We first define real-valued quantities α and β to be the real and imaginary components of γ; i.e., αRe{γ} \[\beta \tr...We first define real-valued quantities α and β to be the real and imaginary components of γ; i.e., αRe{γ} βIm{γ} and subsequently γ=α+jβ Then we observe e±γz=e±(α+jβ)z=e±αz e±jβz It may be easier to interpret this expression by reverting to the time …

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