Chapter 27: Problem 19
For the case of Lecher wires, show that voltage nodes are current antinodes and vice versa.
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Chapter 27: Problem 19
For the case of Lecher wires, show that voltage nodes are current antinodes and vice versa.
These are the key concepts you need to understand to accurately answer the question.
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(a) Show that the equation determining the relative phase can be written as \(\tan \vartheta=\) \(Q\left(\omega / \omega_{0}\right)\left[1-\left(\omega_{0} / \omega\right)^{2}\right]\). Using this, show that, for a given \(\$$, the larger the value of \)Q\(, the smaller the corresponding value of \)\omega\( will be. (b) If the voltage across the capacitor is regarded as a function of frequency, show that its maximum amplitude occurs when \)\omega=\omega_{0}\left[1-\left(1 / 2 Q^{2}\right)\right]^{1 / 2}$.
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There is a real current \(I=I_{0} \cos (\omega t+\epsilon)\) in a circuit consisting of a resistance \(R\) and inductance \(L\) connected in parallel. Find the voltage \(V(t)\) across this circuit.
By assuming that the line parameters themselves are independent of frequency, one can get a "distortionless" line, that is, the propagation quantities are independent of frequency, provided that \(L^{\prime} G^{\prime}=R^{\prime} C^{\prime}\). Show this to be the case by finding \(\alpha, v\), and \(Z_{i}\). (In practice, this generally requires unacceptably large values of \(L^{\prime}\) and/or \(\left.G^{\prime} .\right)\)
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