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the plasma frequency. Its electric field strength falls off at a rate of e^-?d/?d in the direction of propagation along the interface due to two-dimensional geometrical field spreading at a rate of 1/?d, in combination with a frequency-dependent exponential attenuation (?), which is the terrestrial transmission line dissipation, where ? depends on the medium's conductivity. Arising from original analysis by Arnold Sommerfeld and Jonathan Zenneck

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