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#1
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Ok, so trying to summarize your answers, it seems that
- Electric and Magnetic fields, effectively, go together, but their ratio may vary, especially at the antenna's near field. - Cecil Moore says in free space this ratio is the 377 ohms characteristic impedance. I don't know how to mathematically check this, but seems reasonable to me. - It is clear that polarization is an important factor in rejecting noise. I never doubted that. So, apparently, it would be clear that - a reception system capable of discriminating electric/magnetic fields should be able to reduce unwanted noise from near sources and -adding the capability to discriminate different polarizations would also help with noise from both near and far sources. Correct? 73, EA3FYA - Toni |
#2
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Toni wrote:
Ok, so trying to summarize your answers, it seems that - Electric and Magnetic fields, effectively, go together, but their ratio may vary, especially at the antenna's near field. - Cecil Moore says in free space this ratio is the 377 ohms characteristic impedance. I don't know how to mathematically check this, but seems reasonable to me. SNIP Zo = SQRT[u/e] where u = permeability of free space where e = permittivity of free space |
#3
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Your summary seems reasonable, though I'd add one more thing. I
didn't mention the polarization in my first post, to keep things simple. And I didn't mention that you can discriminate also based on direction of propagation. So a highly directional Yagi or parabolic reflector antenna or such can greatly enhance the signal/noise ratio, if the noise is not coming all from the same direction as the signal. And if the noise is coming from only one direction, it's possible to put that direction in the null of a simple antenna with a dipole or a cardiod pattern, such as an electrical dipole or a loop (magnetic dipole). With regard to 377 ohms, it falls nicely out of the physical constants for freespace and Maxwell's equations. If you were embedded in a large block of polyethylene, however, you would see a different ratio, just as the impedance of a coaxial line changes if you change its dielectric from air to polyethylene. About polarization: that works well for signals in freespace. But when you are close to a perfectly conducting plane, the electric field is constrained to be perpendicular to the plane at the surface of the plane. Though it's not a perfect conductor, the surface of the earth tends to keep the electric field vertical in the region where we'd generally put our medium-wave and long-wave antennas...that is, within a fraction of a wavelength of the earth. That's why it's important for a loop antenna to have symmetry about a vertical plane: the so-called "shielded loop" should have its gap at the top (or the bottom, but it's usually easier to have it at the top). This is all explained nicely in King, Mimno and Wing, "Transmission Lines, Antennas and Waveguides." The loop antenna explanation in Johnson and Jasik is also quite reasonable. (There's more to be said about EM wave polarization and the earth, and I suppose others will pipe up and say much of it...) Cheers, Tom Toni wrote in message . .. Ok, so trying to summarize your answers, it seems that - Electric and Magnetic fields, effectively, go together, but their ratio may vary, especially at the antenna's near field. - Cecil Moore says in free space this ratio is the 377 ohms characteristic impedance. I don't know how to mathematically check this, but seems reasonable to me. - It is clear that polarization is an important factor in rejecting noise. I never doubted that. So, apparently, it would be clear that - a reception system capable of discriminating electric/magnetic fields should be able to reduce unwanted noise from near sources and -adding the capability to discriminate different polarizations would also help with noise from both near and far sources. Correct? 73, EA3FYA - Toni |
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