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On Dec 12, 8:44 pm, "AI4QJ" wrote:
"Cecil Moore" wrote in message . net... wrote: Although we know that the 200 ohm line is longer, there is no indication that the length of the 600 ohm line must or must not change. The phase shift at the impedance discontinuity depends upon the *ratio of Z0High/Z0Low*. The following two examples have the same phase shift at the impedance discontinuity. Z0High Z0Low ---43.4 deg 600 ohm line---+---10 deg 100 ohm line---open ---43.4 deg 300 ohm line---+---10 deg 50 ohm line---open So how long does the 600 ohm line have to be in the following example for the stub to exhibit 1/4WL of electrical length? ---??? deg 600 ohm line---+---10 deg 50 ohm line---open Based on what you say above, Zo high/Zo low = 6 resul;ts in 37 degrees. Then for phase shift, (Zo high/Zo low)*37 deg = 6*D where D = phase shift. If the above ratio is literally true, then in the above example, 12*37deg/6 = 74 degrees and length of the 600 ohm line = 90-74-10 = 6 degrees. However, I would like to find a reference for the math showing the characteristic impedance ratio relationship with phase shift. I am reluctant to accepting formulas without seeing them derived at least once. In another thread, "Calculating a (fictitious) phase shift; was : Loading Colis", David Ryeburn has provided the arithmetic for the general case which includes the following expression: -j*(Z_2)*cot(alpha + beta) = -j*(Z_1)*cot(alpha) "alpha" is the length of the open line "beta" is the "phase shift" at the joint "Z_2" is the impedance of the open line "Z_1" is the impedance of the driven line It can be seen, as noted by Cecil, that beta will be the same if the impedances of the two lines are scaled proportionally. But beta is dependant not only on the two impedances, but also on the length of the open line. There are no simple relationships here. It does not seem to be a concept that is particularly useful for the solving of problems. ....Keith |
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