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Walter Maxwell wrote in
: On Sat, 07 Apr 2007 05:03:51 GMT, Owen Duffy wrote: Walter Maxwell wrote in m: On Fri, 06 Apr 2007 23:03:42 GMT, Cecil Moore wrote: MRW wrote: Any comments? Really, what I'm trying to understand here is: if constructive interference does any good in radiowave propagation. I was thinking that with an increase in amplitude the signal would be able to travel a little further, but the signal received may not be accurate in terms of the information it is conveying. Antenna gain over isotropic is an application of constructive interference. The constructive interference must be balanced by an equal amount of destructive interference elsewhere to avoid violating the conservation of energy principle. This is what I've been trying to persuade the 'anti's' that whenthe radiation fields from two vertical dipoles superpose at some point in space, where their magnitudes are equal and are 180° out of phase, the wave cancellation resulting from destructive interference produces a null in a predetermined direction, and thus prevents those fields from propagating any further in that direction. At the precise instant the null is produced, the constructive interference following the principle of energy conservation yields an increase in the field strength in directions away from the null direction. This explains the concept of antenna-pattern modification, and contradicts the notion that the two fields just plow through each other with no effect on either. Walt, this seems inconsistent with the approach that I believe you seem to use in analysing waves in transmission lines where you seem to want to not only deal with the forward and reverse waves separately (ie to not collapse them to a resultant V/I ratio at a point), but to deal with multiply reflected waves travelling in the forward and reverse direction (which is only necessary in the transient state). Owen Owen, it appears that you've misinterpreted my approach. In developing a condition for impedance matching, such as adding a series or shunt stub at the proper place on a transmission line, the object has always been to generate a new reflection at the stub point of the opposite phase to that appearing on the line at the stub point. Thus when the stub reflection and the load reflection superpose at the stub point, the resulting reflection coefficients of voltage and current form either a virtual open circuit or a virtual short circuit. These conditions are produced because when the load impedance is greater than Zo, the resultant reflection coefficient angles at the stub point are 0° for voltage and 180° for current, establishing a virtual open circuit at the stub point to rearward traveling waves. When the load impedance is less than Zo, the resultant reflection coefficient angles are 180° for voltage and 0° for current, establishing a virtual short circuit at the stub point for rearward traveling waves. Hi Walt, I read the above, and I think I can see what you are getting at, however I think it is flawed. If you were to try to extend this method to explain the common two stub tuner (where the length of the stubs is adjustable and the distance between them is fixed), you will have to deal with a situation where the load end stub junction does not present the "virtual o/c or s/c" you describe, your "total re-reflector concept" and you come to need to calculate the situation on the source side of the load end stub (possibly by conventional methods?). Walk your explanation around a Smith chart, and explain why, if the principles on which your explanation are based are correct, why energy fills a 3/4 wave hi Q coaxial resonator rather than being blocked by the virtual s/c or o/c at the first voltage minimum or current minimum. Someone else persuing the theme that reflected waves always travel all the way back to the source, seems to come to a position that some kinds of matching produce a complementary reflected wave, and that really there are two (or more) reflected waves, its just that they have zero net energy. Some of us would accept that if the resultant is zero, there is no wave. Otherwise, you would see a multitude of net-zero waves all around us to complicate every analysis. These "new" and alternative explanations are questionable and don't seem better than the conventional explanations of a transmission line that are set out in just about any reputable transmission lines text. What advantages do these explanation have, who are they targeted at? Is the "total re-reflector" concept to appeal to a dumbed down audience who can get their mind around a bunch of words that describe specific situations in a simple and appealing way, but an incorrect explanation nonetheless? I think it is a real challenge to teach people a simple explanation of what happens without telling them convenient lies that have to be unlearned to develop further. The "reflected wave is (always) dissipated in the PA as heat" is an example of one of those convenient lies. Owen |
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