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Just a few odds and ends. Consider the following which is called a "cascaded line" problem. These are problems where we have two differenttransmission lines, with different characteristic impedances. Since we will give all of the distances inwavelengths,λ, we will assume that theλwe are talking about is the appropriate one for the line involved. Ifthe phase velocities on the two lines is the same, then the physical lengths would correspond as well. The approach isrelatively straight-forward. First let's plot on the Smith Chart . Then we have to rotate so that we can find , the normalized impedance at point A, the junction between the two lines . Thus, we find . Now we have to renormalize the impedance so we can move to the line with the new impedance . Since , . This is the load for the second length of line, so let's find , which is easily found to be , so this can be plotted on the Smith Chart . Now we have to rotate around another so that we can find . This appear to have a value of about , so . There is one application of the cascaded line problem that is used quite a bit in practice. Consider the following: We assumethat we have a matched line with impedance and we connect it to another line whose impedance is . If we connect the two of them together directly, we will have a reflection coefficient at thejunction given by
Thus
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