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Cecil Moore wrote:
Here are some valid conclusions that can drawn from the "Current through coils" thread. A mobile antenna is a standing wave antennas. Some mobile antennas use loading coils within that standing wave environment. There is no useful phase information in standing wave current. Therefore, standing wave current cannot be used to determine the percentage of a wavelength that is occupied by the coil. I think I disagree with this. A standing wave has one of two phases with respect to time, but the two waves traveling through both the antenna elements and any loading coils do have phase shifts, both with respect to time and with respect to position. But when the two waves are superposed, all that is left of this phase information is phase with respect to position. The phase shift of both the single direction waves can be inferred by the shift in position of where they combine to form a node (if you make the (reasonable?) assumption that the delay in both directions is equal. Standing wave current cannot even be used to determine what percentage of a wavelength is occupied by the whip above the coil. There is information about this in the amplitude versus position of the standing wave. But the only very definite points in this variation are the nodes, so is the length is less than a half wavelength, you have only the node at the end to work with, so you have to use the sinusoidal amplitude curve to work with. Standing wave current has virtually unchanging phase the entire length of the mobile antenna. With respect to time, yes. With respect to position, no. The amplitude is different at different locations, so you can use phase of the wave with respect to position. It is just a bit of a mental switch to change from phase in time to phase (fraction of a 180 degree half cycle of amplitude wave from one node to the next). The percentage of a wavelength occupied by any element can be estimated using that element's velocity factor. Or the velocity factor of the traveling waves can be measured by the interference pattern they produce as a standing wave. One cycle of the standing amplitude wave has to occupy the length that carries one cycle of the traveling wave. The velocity factor of the whip is known. Lets say that it has been measured for some cases, and generalized to others. The velocity factor of the coil can be measured or estimated using applicable formulas. If they apply to this particular coil construction. Or you could measure the standing wavelength with an without the coil and, so, measure the coil's "length" in standing wave (and thus, traveling wave) lengths. The presuppositions of the lumped-circuit model render it ineffective in any attempt to analyze large coils in a standing wave environment. Or any other environment where they have a net delay (electrical length) that is not insignificant with respect to the frequency in question. Either the distributed network model or Maxwell's equations must be used to obtain valid analysis results. Or you work with amplitude measurements versus position of the standing wave. |
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