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Walter Maxwell wrote:
On Sat, 07 Apr 2007 16:10:03 GMT, Gene Fuller wrote: [snipped] Walt, Your observation is "correct" only in the case that most people consider for practical reasons. The calculation showing the null behavior is almost invariably performed at infinite distant from the sources, i.e., far field condition. The path from each source to the observation point is considered to be exactly parallel. As you know, there are usually three or more linear dimensions that enter into radiation calculations. In the case of two sources there are four: Wavelength Size of each source Distance between sources Distance to the observation point In the typical "null" presentation, such as that shown in the ARRL publications, the distance to the observation point in always large. Lets take another case, however. Suppose the distance between the sources is some what larger than the wavelength. Make it large enough so there is a region between the sources that would be considered far field from each of the sources. Now calculate the phase differences along some direction from the center point between the sources that eventually points to a null region in the infinite distance. Don't pick an obviously symmetric direction, such as broadside or end-fire, as that would be a special case. What you will find is that when looking at the phase difference along the ultimate null direction is that there is no such null much closer to the sources. The paths from the individual sources are not parallel in this case. The null "line" is actually a curve. The waves pass right through each other in the closer region. The "passing waves" then go on to form nulls in the infinite distance. The nulls in the closer region are not in the same directions as the nulls in the far field. Again, the ground rules: Totally coherent, monochromatic sources Fixed phase difference Far field conditions for each source There are no "tricks" here; this is just a matter of simple geometry. However, it shows that the null you believe demonstrates some permanent interaction and annihilation of EM waves is simply a special case. In classical, non-cosmic, non-relativistic conditions EM waves do not interact in free space. This condition is so widely understood in the scientific world that it becomes a prime candidate for argument on RRAA. 8-) 73, Gene W4SZ Gene, at this point I can't disagree with you. However, in your next to the last paragraph in your post above, if I interpret you correctly, you are saying that all directional arrays, such as are used in AM broadcasting, are considered 'special' cases. Is that what you mean't to infer? Walt, W2DU Hi Walt, Yes, those are special cases, but those special cases are the only ones that most people care about. What I was trying to say might be better illustrated by the following: Two coherent laser beams from the same source can be arranged by suitable mirrors to intersect at some angle. There will most definitely be interference in the region of intersection, but the beams will continue through unchanged. If one measured a beam somewhere downstream from the intersection region it would not be possible to determine that it had crossed another beam earlier. The beams "interfere" but they do not "interact". I know this sounds goofy, and it is critical to keep the definitions straight. When I say the beams do not interact I mean that they do not cause any changes in the other beam. The fact that the beams interfere means that the sum of the fields shows the characteristic constructive and destructive behavior. It does not mean that the waves are henceforth changed. OK, so how does this square with the observation that there are nulls in patterns from two or more RF sources? It is actually very straightforward. In the far field the waves from the separate sources are virtually parallel. Just like Timex, they interfere and they keep on interfering. They never really pass beyond the intersection region. I know it seems like a subtle, or even meaningless, distinction. Do the waves interfere forever or do they actually annihilate each other? For many purposes it does not matter. However, the non-interaction of waves in free space is pretty basic to all of EM analysis. 73, Gene W4SZ |
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