Long Range Propagation of Low Frequency Radio Waves Between the Earth And the Io
Long Range Propagation of Low Frequency Radio Waves Between the Earth And the Io
J Shmoys
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If the dielectric constant is the same function of height as in the preceding section, namely (72) e - 1 ♦ i(YN /cov Q ) e x/h, then the e which appears in the differential equation differs from e by (73) e*-e - -k 2 ^ (e^ •k 2 3 e x 1 e xx r t*2 ~r E In order to simplify the treatment we shift the origin to x • x, defined by x /h (YN /cov o ) e ° - 1 (7U) Z - X - x^ . O - 23 - In terms of z we have then (75) e - 1 + i e z/h, (76) e*-e - k" 2 h" 2 3 1 and therefore sufficiently high frequency.... Forturnately the approximation to the dielectric constant we have been using is valid below ca.
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