The unit vector s was chosen arbitrarily, and ห0 z f L. The precision was set to 1.0 = 10 y3 . For each L, the function T was evaluated at 2 L 2 observation points. This is L in accordance with the demands of MLFMA. The results are presented in Table 2. In the table, entries marked ''direct'' refer
โฆ LIBER โฆ
Microwave imaging of a perfectly conducting cylinder with the use of a simulated annealing approach
โ Scribed by Seon Kyu Park; Cheon Seok Park; Jung Woong Ra
- Publisher
- John Wiley and Sons
- Year
- 1996
- Tongue
- English
- Weight
- 310 KB
- Volume
- 11
- Category
- Article
- ISSN
- 0895-2477
No coin nor oath required. For personal study only.
โฆ Synopsis
In this Letter we suggest an iteratii:e imaging technique based on a simulated annealing (SA) algorithm for a perfectly conducting cylinder. It is numerically shown that an imaging technique that uses SA does not require prior knowledge regarding the center and the shape of an object9 whereas one that uses conuentional gradient algorithms does require this knowledge regarding a scatterer. It is also shown cia numerical simulations thut this technique is very insensitive to noise in the scatteredfield and is not much afpcted by the observaiion locations.
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