modeling of electromagnetic wave scattering and radar cross Ε½ . section, Proc IEEE 77 1989 , 682α699. 3. X. Zhang and K.K. Mei, Time-domain finite difference approach to the calculation of the frequency-dependent characteristics of microstrip discontinuities, IEEE Trans Microwave Theory Tech Ε½ . 36
Validation of the finite-difference time-domain method for near-field bioelectromagnetic simulations
β Scribed by Cynthia M. Furse; Quishan Yu; Om P. Gandhi
- Publisher
- John Wiley and Sons
- Year
- 1997
- Tongue
- English
- Weight
- 183 KB
- Volume
- 16
- Category
- Article
- ISSN
- 0895-2477
No coin nor oath required. For personal study only.
β¦ Synopsis
Figure 8 Reconstruction of a 2-D configuration of small cylinders. Ε½ . Ε½ . a True objects. b Best chromosome of the first generation. Fit-Ε½ . ness s 0.9963340. c Best chromosome of the 500th generation. Ε½ . Fitness s 0.9999881. d Best chromosome of the 1000th generation. Ε½ . Fitness s 0.9999915. e Best chromosome of the 1312th generation. Fitness s 1.0000000 that the converge is accelerated if we use 2-D GA operators, i.e., a 2-D crossover, etc., instead of 1-D operators.
VI. CONCLUSION
An iterative method has been proposed to estimate the width and location of strips. The method is based on a binary LSF combined with a GA. The numerical examples show the effectiveness of the proposed method.
Although the binary LSFαGA method proposed here is applicable to two-dimensional metallic objects of arbitrary cross section, in order to accelerate the convergence rate, it is desirable to improve the GA used here to be suitable for the 2-D objects. This is a topic for future study.
π SIMILAR VOLUMES
Scattering parameters of microstrip ring resonators with ) and without slits that are either edge or side coupled to the feedlines are simulated by the FDTD method. The strip conductors on the de¨ice can either be infinitely thin or finite in thickness. The simulations predict the occurrence of reso
Two different types of source excitation for finite-difference ( ) time-domain FDTD simulations, i.e., electric and magnetic field types, are in¨estigated in this work for configurations that ha¨e no ground planes. This paper shows that the electric field excitation introduces errors in the computed
setup. T h e use of YBa,Cu,O, thin film does not change the antenna design and resonance frequency when compared to a normal metal. At 80 K, the improvement of efficiency was 1.2 d B over a silver counterpart working at the same temperature. This result may be even better at lower temperatures that
and is divided into five uniform segments. For the explicit scheme, the time sample was chosen as 0.053 LM. The Ε½ . current at the location 0.0; y0.1 is shown in Figure 4. Again, the agreement is good, and it is seen that for the implicit scheme, one can make β¬ t large and violate the Courant stabil