Page 270 - Integrated Wireless Propagation Models
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248    C h a p t e r  F o u r


                                     50
                                       �
                                     60
                                             �
                                     70
                                                     �
                                  ill  80                '
                                  :s.                I     '  �
                                  CIJ  90
                                  CIJ                 \
                                  0                   \
                                  �  1 0 0
                                                        '-
                                  Cii
                                  c...  1 1 0
                                                            '
                                    1 2 0                      '
                                    1 3 0
                                    1 4 0
                                      50            1 0 0         1 0 00
                                               Path distance (m)
               FIGURE 4.5.4.2.2  Loss as a function of the distance from the Tx'  e 0, solid line; e 10, dotted
                                                                              =
                                                                 =
                                                                 ,           ,
               line; e 90 dashed line.
                    =
                   ,
               The calculated path loss for a configuration according to Fig. 4.5.4.2.1, with s0 =  100 m,
               s 1  = 200 m, 0 1  = 90 and 0 = 0,10 and 90 degrees is displayed in Fig. 4.5.4.2.2. The param­
                                   2
               eter values q90 = 0.5 and v  = 1.5 is chosen from Eq. (4.5.4.2.3.1). As mentioned earlier,
               the distance dependency of the path loss has two-slope behavior. The first slope is usu­
               ally about 2. After a certain breakpoint distance, x '
                                                         brk
                                       D(x) =J  x: k  '   for x > x brk       ( 4.5.4.2.3.4)
                                            1  1,     for x � x brk

               Then Eq. (4.5.4.2.3.4) is extended according to

                                      L < = 20 log[ 4  n d" o ( "' "   s .   )l   (4.5.4.2.3.5)
                                       "J
                                            -
                                                  ·  -
                                                          £...j=l  J-1 �
                                       dB
                                                   A
               where  i is the physical distance along the path
                     s
                  Equation (4.5.4.2.4) yields a dual-slope path loss curve with a path loss exponent of
               2 for distances less than the breakpoint r and 4 for longer distances.
                                                 b
                  The recursive model is simple and applicable to predicting the microcell signal cov­
               erage. The major microcell propagation effects, such as dual-slope path loss exponents
               and street-corner attenuation, are covered in the model.
               4.5.5  IT - R   P. 1 4 1 1   Model44
                        U
               This model is a popular model issued by the International Telecommunication Union
               (ITU). It consists two parts. One deals with LOS paths and the other with NLOS paths.
               The empirical formulas of this model are explained in this section.
               4.5.5. 1   Definition of Propagation Situations
               In ITU-R P1411, base station BS1  is mounted above rooftop level in a small macro­
               cell environment. Base station BS is mounted below rooftop level in a micro- or
                                             2
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