Page 111 - Integrated Wireless Propagation Models
P. 111

I
                            M a c r o c e  I   P r e d i c t i o n  M o d e I s - P a r t  1 :  A r e a - t o - A r e a  M o d e I s   89
                           1 0  t- � � -- � � .� :: -- ====  �  �  �  � -�-� .� .: .� . � ..  � .� . � .=�1 � :;;= == � �

                                �
                           9 /                          a = 2
                           8        �----�--------------��------�
                                                         1.5
                           7
                           6                              1.0
                         "{ ""  5
                           4                              0.5
                           3
                           2                               0


                                  5   1 0    1 5    20   25   30   35   40   45   50
                                              N u mber of edges n

               FIGURE 2.16.2  Variation of attenuation with number of edges - w  =  150 A.


                  The field A" (a) becomes independent of further increases in n,  as can be seen from
               Fig. 2.16.2. From the results of numerical simulations Walfisch proposed the approxi­
               mate function

                                                          for  n  >  > 1          (2.16.6)


               where  I A I  is the attenuation relative to the free space field strength. This function sug­
               gests a propagation loss dependence of approximately 38 dB I decade of range, which is
               in a close agreement with many reported measurements. This function is I A I  is only an
               approximate, however, and is not a function of n.
                  The overall path loss from the flat-edge model is a summation of three losses: the
               free space loss, the final building diffraction loss, and the reflections from the buildings
               across the street using the Ikegami model, shown as follows:
                                                                                  (2.16.7)
               where L is the free space loss, L is given in Eq. (2.16.1), and L"(t) can be found from
                      F5
                                           E
               Eq. (2 1 6.3).
                    .
                  This formulation is extremely simple to compute and applies for any values of
               angle a, even when the base station antenna height is below the rooftop level. The num­
               ber of buildings can be increased to extremely high values without difficulty.

          2.17    ITU  Model
               It is often difficult to evaluate the best model for a given application from the many
               described in this chapter. Recommendations produced by the ITU are a good reference
               source in this situation, as they summarize in simple form some recommended proce­
               dures, as shown in Table 2.17.1.
                  The ITU's recommendations may not always represent the most accurate model for
               a given case, but they have the benefit of being widely accepted and used for coordina­
               tion and comparison purposes.
                  We'll focus on ITU-R P.1546 and ITU-R P.530 in this section. ITU-R P.1141 is more
               focused on microcells and will be discussed in Chap. 4.
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