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    • 11.3: Co-axial Cables
      https://phys.libretexts.org/Bookshelves/Electricity_and_Magnetism/Book%3A_Applications_of_Maxwells_Equations_(Cochran_and_Heinrich)/11%3A_Transmission_Lines/11.03%3A_Co-axial_Cables
      &\frac{\partial^{2} \text{E}_{\text{r}}}{\partial \text{z}^{2}}=-\mu_{0} \frac{\partial^{2} \text{H}_{\theta}}{\partial \text{z} \partial \text{t}}=\epsilon \mu_{0} \frac{\partial^{2} \text{E}_{\text{...&\frac{\partial^{2} \text{E}_{\text{r}}}{\partial \text{z}^{2}}=-\mu_{0} \frac{\partial^{2} \text{H}_{\theta}}{\partial \text{z} \partial \text{t}}=\epsilon \mu_{0} \frac{\partial^{2} \text{E}_{\text{r}}}{\partial \text{t}^{2}}, \label{11.15}\\ &\frac{\partial^{2} \text{H}_{\theta}}{\partial \text{z}^{2}}=-\epsilon \frac{\partial^{2} \text{E}_{\text{r}}}{\partial \text{z} \partial \text{t}}=\epsilon \mu_{0} \frac{\partial^{2} \text{H}_{\theta}}{\partial \text{t}^{2}}.

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