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Cumulative number of rain storms for which the indicated duration (T R ) has been exceeded in Gera Lario (L), Fucino (F), and Montreal (M).

Cumulative number of rain storms for which the indicated duration (T R ) has been exceeded in Gera Lario (L), Fucino (F), and Montreal (M).

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Article
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We have investigated how rain attenuation statistics, necessary to design fixed satellite systems working at frequencies greater than 10 GHz, are transformed to those applicable to the design of mobile satellite systems working in the same frequency bands and weather conditions in the special case of vehicles driven in zig-zag patterns to simulate...

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... to the satellite so that it always depends on intervals of the true rain-rate space (time) series measured by the fixed observer. Moreover, very unlikely a vehicle will be driven along this orthogonal direction for a significant distance (and time) to experience a constant . The rain-rate field travels rigidly according to its (random) velocity . Fig. 2 shows the cumulative number of rain storms for which the indicated value of has been exceeded for the three sites (once normalized to the total number of rain storms, the curves become the cumulative probability distributions of ). Notice that the value calculated from (1) is at best an estimate of the length of a section, seen by the ...
Context 2
... a given , we can estimate according to (1). As a consequence the curves of Fig. 2, once normalized, give the cumulative distributions of too, e.g., by assuming km/h for Gera Lario and Fucino, and km/h for Montreal. For the latter site, the values of the speed estimated for each single rain storm yields a probability distribution of not significantly different from that calculated with the average ...
Context 3
... conclusion, to estimate we need to calculate the average distance (or, equivalently, the average duration of rain storms, , as ) covered by the fixed terminal and the average distance covered by the vehicles (or the derived parameter ). Let us estimate these parameters. The probability distribu- tion of can be calculated from the curves shown in Fig. 2. Now, Fig. 7 shows the probability distribution of obtained from the simulations. From these curves, we have calculated and , and then from (15), we have derived and , and finally from (14), the corresponding values of . These results are reported in Table ...

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... This involves the calculation of static (i.e., long-term) and dynamic (i.e., short-term) parameters of rain attenuation. A key factor in the conversion of fixed rain-attenuation statistics into mobile rain-attenuation statistics is the velocity factor ξ, defined as [28,29]: ...
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We have presented a picture of the total attenuation to be considered in satellite communication and broadcasting systems in the 10–100 GHz frequency range. Although the findings and methodology are of general interest, the numerical results apply to the Italian (mid-latitude) sites of Fucino and Gera Lario and to slant paths of elevation angles 33° and 32° respectively. The rain attenuation probability distribution P(A), of exceeding the value A (dB) at a given carrier frequency in an average year, has been estimated by the synthetic storm technique and an associated formula, presently derived, which links A to frequency for fixed probabilities. The extra fading due to water vapour, clouds, oxygen and scintillations is estimated by applying the ITU-R formulae. After studying how the received carrier power PR changes as a function of frequency for fixed antenna dimensions and transmitted carrier power PT, we have carried out an exercise to show what first order values of PT we need in an ideal QPSK modulation scheme, with a standard uncoded stream of 64 kbit/s, in a complete earth–satellite–earth connection, with regenerative or transparent transponders, for a given maximum bit error rate tolerated by users. After this analysis we have drawn the following conclusions: (a) the results depend very much on the outage probability and on the site; (b) there are two windows at high outage probabilities, e.g. 1%, the first in the 20–50 GHz frequency range and the second beyond 70 GHz; (c) in the frequency range 50–70 GHz any significant service availability level cannot be achieved because of the very large fading due to oxygen; (d) the transmitted power can show sharp minima which depend significantly on the outage probability and on the site; (e) service availability levels better than 99⋅99% of the year cannot be achieved at frequencies of 30 GHz and above, with ground station antennae of 25 cm or less aperture diameter. © 1998 John Wiley & Sons, Ltd.