Enthalpy
12th July 2008 - 01:30 AM
I guess you got your information from
http://en.wikipedia.org/wiki/Schumann_resonancesnot a very clear entry.
I could indeed imagine a very slow (under 5kHz) resonance involving the soil and the ionosphere. The lowest mode would have a + potential at the soil at one place, a - at the ionosphere above that place, a - at the soil at the antipode and a + at the ionosphere at the antipode. And of course, slow currents flowing in the soil and - in opposite direction - in the ionosphere between the electric poles.
The resonant frequency doesn't depend on the soil-ionosphere distance (which doesn't act as a waveguide in this case, since its cutoff or minimum frequency is around 5kHz) because this distance increases the inductance as it reduces the capacitance equally.
You can compare this fundamental mode to a very short and broad coaxial line with its central conductor (= the soil) open at both ends.
The fundamental resonant frequency would be about half a vacuum wavelength in 20.000km or 7.5Hz. No need for refractive materials.
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Earth used as an antenna in ELF: we have little choice! Antennas must be huge, so they must be horizontal and are unavoidably near to the soil. A perfectly conductive soil would efficiently cancel the signal received by the antenna's wire (put another way: the wave induces the same voltage in the wire and in a conductive soil, so you see no voltage difference at the ends), but the trick is that the soil is lossy. By grounding the wire at its far end, you get a voltage at the near end which corresponds to the losses by the current induced in the soil.
So: no relationship to the iron core nor refraction.
It is an equivalent to the "transfer impedance" of a coax cable. The induced parasitic voltage is due to te losses in the shield.