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parameter F . If the distance between the edge and the MS is now large, the MS must move over a large distance (e.g., several tens of wavelengths) for the eld strength to change noticeably. Note that this effect changes the absolute amplitude of the MPC, |a|, and has nothing to do with an interference effect. Consider now the situation where an MPC undergoes several of these or similar processes on its way from the TX and RX, each of which contributes a certain attenuation. The received eld strength then depends on the product of the attenuations; on a logarithmic scale, these attenuations add up. We can thus model the effect as the sum of random variables on a dB scale i.e., a lognormal distribution. However, the mechanism just described is not necessarily valid in all physical situations.8 Consider now the statistics of the eld strength based on samples taken from a large area (i.e., including both lognormal fading and interference effects). The pdf of these samples is given by the so-called Suzuki distribution, which follows in a straightforward manner from the laws of conditional statistics. The mean value of the eld strength, taken over a small area, is r = /2, and the distribution of the local value of the eld strength conditioned on is pdf (r|r) = r 2r 2 exp r 2 4r 2 (5.60) c# split pdf How to convert "PDF TO IMAGE" in c# ? - C# Corner
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