Page 391 - Integrated Wireless Propagation Models
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                  T h e  l e e  C o m p r e h e n s i v e  M o d e  - 1  I n  e   g r a t i o n  o f  t h e  T h r e e  l e e  M o d e I s   369
               6.4.2.2  Finding RSSI at Point 7
               Point #7 is located outside the building. Along the radio path from the transmitter to the
               receiver point 7, we use the inter-building formulas shown in Eq. (5.3.4 .. 3.2):

                                                                                (5.3.4.3.2)


               where 8 is the incident angle between the external building wall and the wave path.
               When e = 90°, the wave is perpendicular to the wall, and when 8 = 0°, the wave is at
               perfectly grazing conditions.
                  5 1  is the first segment of the distance (path) from the transmitter inside the building to
                                              2
                                      {./ 2
               its building wall, that is, 51 =  25 + 45 = 51.5 m. The path-loss slope m is assumed 20 dB/
               dec because it is in a free space condition.
                  The  second  segment  of the  distance  is the  outside-building  distance  5 to the
                                                                                 2
                                           2
                                      2
               receiver, which is about  {./ 30 + 25 = 39 m. Since the radio wave passes through just one
               wall, a path loss causes by one wall (at 8 = 90°) is about 10 dB, that is, L ,  = 10 dB. Lee is
               an additional loss when the incident angle 8 = 0°. Usually, Lee = 20 dB. In this case, as
               shown from Fig. 6.4.2. ( a), e = 135°. Thus, from Eq. (5.3.4.3.2),
                                  1
                                            + 20 log (51 + 5 ) + Le + L (1 - sin 8) 2
                         L = 32.4 + 20 log  (J GHz)     2       c,
                           = 32.4 + 20 x log (2.4) + 20 log (51 . 5 + 39) + 10 + 20 (1 - sin 135°) 2
                           = 32.4 + 7.6 + 39 1   + 10 +  . 1 7 5 = 90.27 dB
                                        .
                                               1
               The RSSI at point 7 is

                                Transmitter power (0 dBm) - L = -90.27 dBm



               6.4.2.3  Finding RSSI at Point 13:
               Point #13 is located in the another building. Along the radio path from transmitter to
               the receiver at point 13, the first segment 5 1  of the distance (path) is the distance from
                                                                       2  2
               the transmitter inside the building to its building wall, that is, {./ 25 + 9 = 26.57 m.
                  The second segment 5 of the distance is the outside distance, which is about
                                      2
                      2
                            2
               �(  45- 9) + 100 = 106.28 m. The radio wave in this case passes through 2 walls, each
               wall causes about 10 dB loss, 2L ,  = 20 dB
                  The third segment 5 of the distance is from the outside wall of the receiver building
                                   3
               to the receiver inside the building, which is about 10 m. The free-space path-loss slope
               of 20 dB/dec is assumed. Also, LGe has a default number 20 dB. The incident angle
                     1
               e = tan- ( �)  = 19.8° can be found from Fig. 6.4.2.1(a).
                       1 5
               The total loss L calculated from Eq. (5.3.4.3.3) is
                   L = 32.4 + 20 log  (J GHJ + 20 log (5 1 + 5 + 5) + 2L ,  + L (1 - sin 8) 2
                                                               c,
                                                  2
                     = 32.4 + 20 log (2.4) + 20 log (26.57 + 106.28 + 10) + 20 + 20 (1 - sin 19.8°) 2
                     = 32.4 + 7.6 + 20 log (142.85) + 20 + 20 x (0.661) 2
                     = 32.4 + 7.6 + 43 + 20 + 8.73 = 111.73 dB
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