Page 263 - Integrated Wireless Propagation Models
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                                                           M i c r o c e  I   P r e   d i c t i o n  M o d e I s   241






                                  ,'D   -  -  - -  -  -  - [LdJ - l- -  -  -  -  -  ,•- Average
                                                          -
                                                 -

                             ¢�1  r  I                       l  i � \ �:�:,,

                            /        as                             as     �
                                     ...,__ -  -  -  -  - - - 1   �;:  � - - - -  -  -  - -  � � Receiving
                                            -
                 Transmitting �  _  _  _
                 antenna                                                1      antenna
                                                                        RG waves

               FIGURE 4.5.2.2.2  M u l ti path propagation model i n   a high-density urban area.




                  In the microcell environment, a street-guided wave exists, at least in the immediate
                                                                                       2
               vicinity of the transmitter. From a result of their measurements, Kaji and Akeyama 3
               suggested an empirical model in the form:


                                                                                (4.5.2.2.1)

               for base antenna heights in the range of 5 to 20 m and for distances between 200 m and
               l km. In this equation,
                  S  t he signal level (dB V),
                    =
                                     �
                  d = the distance from the transmitter,
                  a =   the basic attenuation rate for short distances (approximately l),
                  b = the additional attenuation rate for distances beyond the turning point,
                  g = the distance corresponding to the turning point, and
                  c = the offset factor.
               The model has two limiting cases. In case 1, for distances significantly less than g, the
               attenuation is such that
                                                                                (4.5.2.2.2)
                                            S = -20 log d" + c
               In case 2, for distances greater than g, the attenuation falloff rate tends to be such that
                                                   b)
                                                  n
                                      S = -20 log d < + + c + constant          (4.5.2.2.3)
               This model was fitted from their measured results at 900 MHz; the values for the vari­
                                                 1
               ous coefficients are given in Table 4.5.2.2. .
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