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Reg Edwards wrote:
For those of you who may be unfamiliar with the mathematics of transmission lines, download program TWOLINES and enter the following practical values - Line-1 represents the loading coil. Line-2 represents the whip to be pruned for 1/4-wave resonance. Enter Zo1 = 6000 ohms, a practical value. Enter electrical length L1 = 0.15 wavelengths. Enter attenuation = 0.1 dB for wire loss in coil. Ignoring losses and starting at 0-j0, plotting this value on a Smith Chart normalized to 6000 ohms, the normalized value is -j1.38 -j1.38 * 6000 = -j8280 ohms Enter Zo2 = 400 ohms, a practical value. Enter electrical length L2 = 0.0077 wavelengths. Enter attenuation = 0.001 dB Starting at 0-j*infinity and plotting backwards, this value on a Smith Chart normalized to 400 ohms is -j20.7 -j20.7 * 400 = -j8280 ohms But L1 + L2 = 0.1577 wavelengths = only 57 degrees. The abrupt jump from -j1.38 to -j20.7 provides a 66 degree phase shift in the angle of the reflection coefficient as read off the Smith Chart. The missing 90 - 57 = 33 degrees are just not needed for resonance. So why is everybody making such a fuss about it? The missing 33 degrees are there, provided by the phase shift in the reflection coefficient. The angle of the reflection coefficient in the stinger at the impedance discontinuity is ~6 degrees. The angle of the reflection coefficient in the coil at the impedance discontinuity is ~72 degrees. 72 - 6 = a 66 degree jump in the angle of the reflection coefficient. That equates to the missing 33 degrees of antenna. The wave that is only 3 degrees back from the tip reflection point is suddenly only 54 degrees from the current maximum point. It appears to me that the interference of the forward and reflected waves at the impedance discontinuity causes an actual 33 degree phase shift. How to analyze what happens at such an impedance discontinuity is covered in my energy analysis article at: http://www.qsl.net/w5dxp/energy.htm I will try to do that analysis sometime today. -- 73, Cecil http://www.qsl.net/w5dxp |
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