We begin by differentiating both sides of Equation \ref{m0027_eTelegraphersEquation1p} with respect to z, yielding: \[-\frac{\partial^2}{\partial z^2} \widetilde{V}(z) = \left[ R' + j\omega L' \ri...We begin by differentiating both sides of Equation \ref{m0027_eTelegraphersEquation1p} with respect to z, yielding: -\frac{\partial^2}{\partial z^2} \widetilde{V}(z) = \left[ R' + j\omega L' \right]~\frac{\partial}{\partial z} \widetilde{I}(z) \nonumber Then using Equation \ref{m0027_eTelegraphersEquation2p} to eliminate \widetilde{I}(z), we obtain \[-\frac{\partial^2}{\partial z^2} \widetilde{V}(z) = -\left[ R' + j\omega L' \right]\left[ G' + j\omega C' \right]~\widetilde{V}(z) \n…
We begin by differentiating both sides of Equation \ref{m0027_eTelegraphersEquation1p} with respect to z, yielding: \[-\frac{\partial^2}{\partial z^2} \widetilde{V}(z) = \left[ R' + j\omega L' \ri...We begin by differentiating both sides of Equation \ref{m0027_eTelegraphersEquation1p} with respect to z, yielding: -\frac{\partial^2}{\partial z^2} \widetilde{V}(z) = \left[ R' + j\omega L' \right]~\frac{\partial}{\partial z} \widetilde{I}(z) \nonumber Then using Equation \ref{m0027_eTelegraphersEquation2p} to eliminate \widetilde{I}(z), we obtain \[-\frac{\partial^2}{\partial z^2} \widetilde{V}(z) = -\left[ R' + j\omega L' \right]\left[ G' + j\omega C' \right]~\widetilde{V}(z) \n…
