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               FIGURE 5.6.2.2.3  Data model for FDTD simulation. (A color version of this figure is av i l able at
               www.mhprofessional.comjiwpm. )


                                                   t
                                                                            o
               can  o   the iterations within one time step  o   gain all the E and H values  f   all the cells
                  d
               or grids. Since the iteration is processing one by one in time steps, we can reach any
               time's state of the whole system after repeating the same procedure. This is the key part
               of the FDTD procedure. The initial E and H are equal to zero when the procedure starts
               from the very beginning. Therefore, we may not need to start at the very beginning. If
               we have knowledge of the past and current state of the system at any time point, we can
               start from that time point to predict the future state of the system. The iterations make
               up the procedure of the FDTD.
                  Figure 5.6.2.2.3 shows the data model for the FDTD calculation obtained from a
               picocell. Based on the input data, the FDTD can calculate the expected values for each
               point. Again, this depends on how much detail and on the granularity to derive the final
               value. Figure 5.6.2.2.4 shows electromagnetic field simulated using the FDTD technique.
               The electric field is strong at the corner of the picocell, as shown in Fig. 5.6.2.2.4.

               5.6.2.3  3 D   Ray-Tracing and FDTD Models versus the Lee Model
               In this case, the 3D ray-tracing and FDTD models were implemented in the same sce­
               narios for comparison with the Lee Model. The room is assumed to have a uniform
               dielectric environment, and the simulation was done for just one room case-the second
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               floor of north wing at Republic Polytechnic (RP) in Singapore (see Fig. 5.3.2. . 2).
                  The deviation is the difference between the predicted and the measured values, as
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               shown in Fig. 5.6.2.3. .   As shown, the ray tracing (with and without furniture) and Lee
               models gave a decent prediction in this scenario. However, the FDTD model did not
               show its performance to be as good as that of the other two models. The main possible
               reason is that the 1 x 1 m-square grid is too large to be accurate for the FDTD model in
               this case. Furthermore, with the consideration of furniture, the gird should be even
               smaller. This is also the reason that applying the FDTD model in a furnished room here
               gives the worst performance. However, as we mentioned earlier, if we put more com­
               putational resources into the FDTD model, the results should be better.
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