periodic structure. The second (see is that there is very good agreement between the results obtained using the ADI-FDTD method and the conventional FDTD method, but the ADI-FDTD method is faster than the conventional FDTD method because the longer period of time is utilized. The last observation made from Figure 4 is that a nearly perfect reflection is achieved in the frequency range from 250 -350 MHz.
CONCLUSIONIn the conventional FDTD method, the maximum time-step size is limited by minimum cell size in the computational domain. Certainly, a small time-step size will lead to a significant increase in calculation time so that the advancement time velocity will be relatively slow. In this paper, the restriction of the time-step size in the conventional FDTD method is removed by employing the ADI technique. For periodic problems such as PBG materials and spiracle cavities, the resonance phenomenon is engendered easily. Therefore, the ADI technique is an effective means for solving these kinds of abovementioned periodic problems. Compared with the conventional FDTD method, the ADI-FDTD method is found to be fast when the same accuracy is kept. As an initial work, we started with the 1D case only, but in the future it can be extended to multidimensional problems.