Page 314 - Integrated Wireless Propagation Models
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                  Between these two wings, there is a corridor junction, which is 8 x 10 m in length
               and width, as shown in Fig. 5.3.2.0.2. On each floor, the brick walls were used to divide
               several classrooms (three classrooms in the north wing and three classrooms in the
               south wing) and an aisle. The furniture in the classroom includes school desks and
               chairs, which were made of plastic and reinforced metal brackets. Both the north and
               the south sidewalls were full of windows. There were three access points (AP) in the
               north and south wings on each floor. The three APs were operational on three signal
               channels: channels 1, 6, and 11. The APs were mounted fixed at a height of  . 5 m.
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               5.3.2. 1    A Same-Floor Case
               Figure 5.3.2.1.1 shows a top view of south wing and the locations where the signal
               strengths were measured and the locations of APs. On the same floor, we took the mea­
               surements on each floor from the second to the fourth floor. On every floor, nine APs are
               shown, and 18 spots were picked up to measure the signal strength. The positions of
               these spots are the same for each floor.
                  In Figs. 5.3.2.1.1 and 5.3.2.1.2, the green circles represent the desks and the sur­
               rounding blue circles are chairs. The red rectangles represent the measurement points.
               The yellow bars on each side of the building are windows, and the black bars are the
               doors. The frequencies are transmitted on channels 1, 6, and 11 on 802.11b. Some pic­
               tures were taken to correlate the measured data with the environment. The red arrows
               indicate the directions of the camera.
                  Figure 5.3.2.1.2 shows a top view of north wing and the locations where the signal
               strengths were measured as well as locations of APs. The layouts for both south and
               north towers are almost the same. Both have nine APs and many windows on each
               floor. The divider in each floor is almost the same as well. Two towers are connected
               with a corridor. This makes radio planning extremely difficult.
                  In Fig. 5.3.2.1.2, we divided these points into two groups: one belongs to the LOS,
               and the other belongs to the NLOS. P2 , P4, and P6 were transmitted into NLOS areas.
               The rest APs were transmitted in the LOS areas. As there are APs on both sides of the
               building inside and outside the room, it is difficult to mark these measurement points
               as LOS and NLOS in Figs. 5.3.2.1.1 and 5.3.2.1.2. The Lee model uses these points to
               calculate the prediction of path loss. For the LOS case, the loss can be calculated from
               Sec. 5.2.2.1 .
                           o
                  The slope  f   the interior wall loss  s   derived through the standard integration pro­
                                               i
               cess of measurement, as shown in Fig. 5.3.2. . 3. The slopes of wall loss from both wings
                                                    1
               of the building were obtained from the best fit of the measured data. It replaced the old
               value of  min wall in Eq. (5.2.8.3.2). Then the new value was used to calculate the prediction
               values.
               5.3.2.2  An lnterfloor Case
               Measurement data were also collected from the nine APs at different floors and different
               wings.
                  The locations of the measurement spots and the APs are exactly the same as we
               used in the same-floor case. The APs were fixed at one side of the ceilings (south side of
               north wing and north side of south wing), while the test spots were spread all around
               on each floor, as indicated in Fig. 5.3.2.1.2. In general, we believe that the interfloor
               propagation is a combination of diffraction and penetration.
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